27

Meson SummaryTable LIGHT UNFLAVORED MESONS

(S=C=B--O)

ud, (u-~-dd)/./2, d-d; forl = 0 (rl, rl', h, h',w, 4, f, f'): Cl(UU + dd) 4- c2($~ ) For / = 1 (~r, b, p, a):

E9

I G ( j P)

= 1-(0-)

II

FI

Mass m = 547.30 • 0.12 MeV Full width r = 1 , 1 8 • 0 . 1 1 k e V [ f ]

(S=

7r+Tr-~r 0 7r+Tr-~r 0 7r+Tr-Tr 0 ~+7r-3`

Left-right asymmetry Sextant asymmetry = Quadrant asymmetry Left-right asymmetry

= (0.09 • 0.17) x 10 - 2 (0.18 • 0.16) x 10 - 2 = ( - 0 . 1 7 • 0.17) • 10 - 2 = (0.9 • 0.4) • 10 - 2

~r+~-7

f l (D-wave) = 0.05 • 0.06

(S = 1.5)

Dalitz plot parameter ~~176176 c~ = - 0 . 0 3 9 • 0.015 DECAY MODES

0.017 9 0.008 0.0116 • 0.0016 R - 0 nKQ+0.009 ..... -0.008

Neutral modes neutral modes 23' 370

~r- modes are charge conjugates of the modes below. P Confidencelevel (MeV/c)

Fraction ( r i / r )

p,+/,'/j /4+ 1,'/~7

[b] [c]

e+Ue e+Ue3"

[b] [c]

D9.987704- 0.00004) % 2.00 :::0.25 ) x 10- 4

e+l/e~r 0 e+vee+e -

e+Z,'eU~

<

1.230 1.61 1.025 3.2 5

30

::s ) x 10- 4 ::=0.23 ) x 10- 7 • ) x 10- 8 /:0.5 ) x 10- 9 x 10- 6 90%

70 70 4 70 70

L

LF

[d] < [d} <

1.5 8.0

p,+v e #-e+e+u

LF

<

1.6

r•

iG(jPC)

x 10- 3 90% x 10- 3 90% x 10- 6 90%

1-(0

27 e+e-3' 3'positronium

(98.798 • (1.198• ( 1.82 • ( 3.14 • ( 6.2 • < 2 [e] < 8,3 < 1.7 < 3.1

e+e+e-e e+e 43' u~ Ue~ e zJ#~# UT~ r

<

2.1

% % ) x 10- 9 ) x 10- 5 )xlO -8 x 10- 8 x 10- 7 x 10- 6 x 10- 6

5=1.1 S=1.1

CL=90% CL=90% CL--90% CL=90%

67 67 67 67 67 67 67 67 67

x 10- 6 CL=90%

67

Charge conjugation (C) or Lepton Family number (LF) violating modes 33' 4- e - # +

<

2.8

%

274 178 257

CL=90%

-

C h a r l ~ modes charged modes /r + ~r- ~r0 7r+ ~r-- 3` e+e-3' /~+/~-3' e+ e -

(28.3 4-0.4 ) % (23.0 4-0.4 ) % ( 4,754-0.11)% ( 4.9 4-1.1 ) • 10- 3 ( 3.1 4-0.4 ) x 10- 4 < 7.7 x 10- 5 ( 5.8 4-0.8 ) x l O -6

~+~r-e+e

5=1.2 S=1.2 S--1.1

CL=90%

252

( 1.3 4-1,2 ) x 10 -3 --0.8

-

Ir+ 7 - 23' ~+7r-/[03' ~[0/~+/~- 7

< < <

2.1 6 3

• 10 -3 • 10 -4 x 10 -6

173 235 274 252 274 235

CL--90% CL-gO%

235 173 210

235

Cha~e conjugation (C), Parity (P), CharKe conjugaUon x Parity (CP), or Lepton Family number (LF) violating modes

Scale factor/ P Confidencelevel (MeV/c)

Fraction ( r i / r )

s=1.2 S=l.1 S-1.2

( 7.1 +1.4 ) x I0 -4

other neutral modes

- 4-)

Mass m = 134.9766 • 0.0006 MeV (S = 1.1) m~r• - m~o = 4.5936 ~: 0.0005 MeV M e a n l i f e r = ( 8 . 4 • 0.6) x 10 -17 s (S = 3.0) c~- = 25.1 nm :r0 DECAY MODES

~r023'

#+#-

30 30 30

(71.6 • )% (39.33• % (32.24:50.29) %

If]

30

Lepton Family number (LF) or Lepton number (L) violating modes P'+Pe

Scale factor/ p Confidencelevel (MeV/c)

Fraction ( r i / r )

(S = 1.3)

Ir+ DECAY MODES

+)

1.8)

t'J=v3f form factors [a]

FV = FA =

#+e-

= 0+(0-

C-nonconserving decay parameters

Mass m = 139.57018 • 0.00035 MeV (S = 1,2) Mean life T = (2.6033 :~ 0.0005) x t 0 - 8 s iS = 1.2) c r = 7.8045 m x :1: ~

IG(J PC)

C

<

3.1

x 10- 8 CL=90%

67

LF

<

1.72

•

26

-8 C L = 9 0 %

lr +'If-

P,CP

<

3.3

x 10- 4

CL=90%

Ir0 Ir0

P,C P

<

4.3

x 10 -4

CL=90%

-

33'

C

<

5

x 10- 4

CL=95%

274

7rOe+e -

C

[g} <

4

x 10 -5

CL=90%

257

7rO/~+/~-

C

[g] <

5

x 10 -6

CL=90%

210

I~+ e- + t~- e+

LF

<

6

x 10- 6

CL=90%

263

l Mass m = (400-1200) MeV Full width r = (600-1000) MeV ro(4OO--120o) DECAY MODES

Fraction (ri/r)

/r 7r 77

dominant seen

p (MeV/c)

28

Meson SummaryTable I p(770)

C h a r l ~ c o ~ u r , d'Jon (C),Padty(P), Lepton~ml~ number(LF)violating modes

IG(jPC) = 1 + ( 1 - - )

[/] I

M a s s m = 769.3 4- 0.8 MeV ( 5 = 2 . 1 ) Full width r = 150.2 4- 0.8 M e V Fee = 6.77 4- 0.32 keV /1(770) DECAY MODES

Fraction ( r i / r )

7/7/

~

100

Scale factor/ p Confidence level (MeV/c) %

358

p(no)9 decays 7/1"4.7 7/4.~/ 7/4.7/4.~T--7/0

( <

<

4.5 4.0.5 ) x 10 - 4 x 10 -3 2.0 X 10-3 6

S=2.2 CL=84% CL=84%

372 146 249

7f+7/~07/0

P.CP P.CP

7e+e 7/0e+ e ~/e+e 37 # + # - 7/o #+#-~/

C C c C c C

e#

LF

( 9,9 4.1.6 ) x l 0 - 3 ( 6.8 4.1.7 ) x 10-4

f/7 [j] [j']

/~+#-e+e7/+ 7/- 7/0 7/+~r 7/+/r-- ~..0 7/0

( 2.4 +0.8 --0.9 ) x 10 - 4 (4.604.0.28) x 10-5 (4.494.0.22) x 10- 5 < 1.2 x 10-4 ( 1.8 4.0.9 )xlO -5 < 4 x 10 - 5

IG(j PC) =

Ci=90% CL=90%

7/7 7/~ e7/0#+~e+e 7/+7/-7/07/0 7r+ 7/--3' Ir + 7/- 7/+ 7/-7/07/07 ~+#-33'

f0(980) DECAY MODES

Fraction ( r i / r )

7/7/ KK

dominant seen

f/7/0 37/0

Scale factor/ p Confidence level (MeV/c)

< <

Charge conjugation (C) violating m o d e s c < 1 x 10 - 3 C < 3 x 10 - 4

Fraction ( r i / r )

77~1" KK 9'7

dominant seen seen

Mass m = 957.78 4- 0.14 MeV Full width F = 0.202 4- 0.016 MeV

~(gras) DECAY MODES 7/+7/--/'/ p~ nonresonant 7/+ ~r- 3') ~T07/0g u)7 77 37/0 /~+/~-- 3` 7/+ 7/--7/0 7/0p0 7/+ 7/+ 7/ 7/ ~ + 7/+ 7/-- 7/-- neutrals 'It + 7/+ 7/-- "/I--- ~0 6/r = + 7 / - e+ e 7f077 47/0 e + e-

Mass m = 1019.417 4- 0.014 MeV

5=1,1 CL=90% CL=95% CL=90% CL=90% CL=95%

CL=90% CL=90%

199 379 349 391 261 365 256 367 376 391

162 329

(S = 1.3) Scale factor/ P Confidence level (MeV/c)

(44.3 4.1.5 ) % (29.5 4.1.0 ) % (20.9 • )% (3.03--0.31) % (2.124.0.14) % (1.564.0.26) x 10 - 3 (1.044.0.26) x 10 -4 < 5 % < 4 % < 1 % < 1 % < 1 % < 1 % < 6 xlO -3 < 8 x 10 -4 < 5 x 10 - 4 < 2,1 x 10 - 7

S=l.2 S=l.2 S=1.2 S=l.3

CL=90% CL=90% CL=90% CL=95% Ct=90% CL=90% CL=90% CL=90% CL=90% CL=90%

232 169 239 160 479 430 467 427 118 372 298 189 458 469 379 479

p (MeV/c)

0-(I--)

(S = 1.8)

Full width F = 4.458 + 0.032 MeV

4(1020) DECAY MODES

(49.2

::EO.7 ) %

~e+e-

1.3

wT/0

7.5 4.8 < <

+0.8

-0,6 4.1,4 4.2.0

4.1,3

( 3.4 4.0,4 ( 1,08 4.0.19 <

8.7

~~ ao(980)7

1.5 1.2 ( 8.6 < 5

I/'(958)7

( 6,7

< <

2 (1,4 < 5 < 3

4.1.8 +3.5 --3.1

<

P77

I h1(1170)I

s=1.4 S=1.2 S=1.2

4.0.5

127 110 363 501 510 499

) • 10-4

363

) x 10- 5 ) x 10 - 5

490

% CL=84% x 10- 5 CL=90%

5 1.2

( 4.1

#+#-7

S=1.2 $=1.2

(33.8 :t:0.6 ) % (15.5 +0.6 ) % 1.2974.0.033) % 1.26 4.0.10 ) • 10 - 3 2.91 4-0.07 ) x 10 - 4 3.7 4.0,5 ) x 10 - 4

e+e #+/~-

f0(980)7 7/~ 7r~ 7 7/+ 7 r - / r + 7/7/+ 7 / + / r - ;T- 7/0 7/Oe+ e-

Scale factor/ p Confidence level (MeV/c)

Fraction ( r / j r )

K+K o o KLK S pTr + ~+7/-7/0 717

P7 ~+ ~-.).

0 + ( 0 - +)

Fraction ( r i / r )

1-(0++)

321 492

I6(j PC) =

w3`

IG(jPC) =

322 479 445 274

470 -

a0(gao ) DECAY MODES

5.3 -3.5 +8.7 ) x 10- 3

< < <

469

p ( M eV/c)

IG(jPC) =

=10(980) [k} I

327 379 365

6.5 4-1.0 ) x 10 -4 5.9 4-1.9 ) x 10 -4 9,6 4.2.3 ) x 10 - 5 7,074.0,19) x 10 - 5 2 % 3.6 x 10- 3 1 x 10- 3 7.2 4.2.5 ) x 10- 5 1.8 x 10- 4 1.9 x 10- 4

458 459

M a s s . = 9 8 4 . 8 4 - 1.4MeV ( S = 1.7) Full width F = 50 to 100 MeV

(88.8 4.0.7 ) % 8.5 4.0.5 ) % 2.21 + 0.30) %

neutrals (excluding7/~

CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90%

IG(jPC) = 0 + ( 0 + + )

369 384 319 246 252

0-(1 --)

Fraction ( r i / r )

7/+7/--7/0 7/03' 7/+ 7/--

x 10-4 x 10-4 x 10-3 xlO -3 x 10 -4 xlO -5 x lO - 5 x 10 - 4

189

Mass m = 782.57 -I- 0.12 MeV (S = 1,8) Full width F = 8.44 4- 0.09 MeV Fee = 0.60 4- 0.02 keV ~(782) DECAY MODES

%

9 9 1.4 2.4 1.0 6.0 is 4.7

Mass m = 980 4- 10 MeV Full width r = 40 to 100 M e V

358 372 S=1.6

< < [g] < [g]< < [g]< [g] < <

I f0(cj80) Ik] I

p('no) o decays 7/+7/-7 7/07

< 2

x 10 - 5 x 10- 4 x 10- 4 x 10 - 4 x 10 - 4 x 10- 4 x 10 - 5 x 10- 3

CL=90% CL=95% CL=90% CL=90%

210 219 490 39 492 410 341 501 346 36

) x 10 - 5 x 10- 5 CL=90% )x10 -5 x 10 - 4 CL=90% x 10 - 4 CL=90%

IG(J PC) = 0 - ( 1 + - )

Mass m = 1170 4- 20 MeV Full width F = 360 -I- 40 MeV h1(1170 ) DECAY MODES

Fraction (l'i/F)

p7/

seen

p (MeV/c) 310

29

Meson SummaryTable

Jb1(1235)J

IG(JPC) =

M a s s m = 1229.5 4- 3.2 MeV Full width F = 1 4 2 • MeV b1(1235 ) DECAY MODES

16(jPC ) =

1+(1 + -)

(S=1.6) ( S = 1.2) p Confidence level (MeV/c)

Fraction ( r i / r )

dominant [DIS amplitude ratio = 0.29 4- 0.04] 7r+-'y (1.6+-0.4) x 10 - 3 f/p seen ~r+ / r + 7r-/r 0 < 50 % ~r0

<

8

%

K 0 K 0/r+-

<

6

%

K~ K~.+

<2

~r

<

348

% 1.5

+)

Mass m = 1297.0 4- 2.8 MeV Full width F = 53 4- 6 MeV

UP~1"

(KK)•

0+(0-

%

84% 90% 90%

608 536 248 238

90% 84%

238 146

II(I~JS) DECAY MODES

Fraction (l'i/F)

T/~1-+

a0(980 ) lr T/~-0 ./r0

seen seen seen

408 245 -

~/(TrTr)s.wave

seen

-

~r -

p (MeV/c)

IG(j PC) = 1 - ( 0 - +) Mass m = 1300 4- 100 MeV [m] Full width F = 200 to 600 M e V

J a1(1260)

I6(j PC)=

[t] J

1 - ( 1 + +)

Mass m -- 1230 ~c 40 MeV [m] Full width F = 250 to 600 MeV a1(1260 ) DECAY MODES

Fraction ( r i / r )

( p'K ) S-wave

seen seen seen seen seen not seen seen seen seen not seen seen

(p~T)D_wave (p(1450) ~T)S-wave (p(14-50) ~r )D-wave o" 71" f0(980) ~r f0(1370) ~r f2(1270) ~r K K * ( 8 9 2 ) +C.C. ~r(13OO)~r ~r 7

p (MeV/c) -

Fraction ( r i / r )

plr ~r (~rlr)s_wave

seen seen

J a2(1320) J

-

p~" T/Tr uJ ~__;T K K T/'(958)~r

-

607

406 --

IG(j PC) :

1--(2

+ +)

Full width i- = 107 4- 5 MeV [m] a2{1320 ) DECAY MODES

-

p (MeV/c)

Mass m =1318.0 4- 0.6 MeV (S= 1.1)

-

Scale factor/ p Confidence level (MeV/c)

Fraction (Fi/r) 470.1 +2.7) (14.5+-1.2) (10.6+-3.2) (4.9+-0.8)

% % % %

S=1.2 S=1.3

(Sm3~Omg) X 10 - ~

~+-7

(2.8+-0.6) (9.4+-0.7) < 8 < 2.3

"y')" /r + T r ~T e+e-

I6(J PC) = 0+(2 + +)

J f2(1270) J

Ir(1300) DECAY MODES

x 10 - 3 x 10 - 6 % x 10 - 7

CL=90% CL=90%

419 535 362 437 287 652 659 621 659

Mass m = 1275.4 4- 1.2 MeV Full width r --- 18~~ ~~+3.4 MeV f2(1270) DECAY MODES

(S = 1.5)

484.7 +2.4

-1.3 )% 7.1 _+~:~ ) ~

S=1.3

622

S=1.3

562

f0(1370) DECAY MODES

Fraction

S=2.8 S=1.2 S=2.4

403 559 327 564 637 475 293 637

~r/r

seen seen seen seen seen seen seen seen seen not seen

7r+ 7r- 2~r0

K~

3"7 ~/';,c';r

<

4.6 ::0.5 ) % 2.8 +-0.4 ) % 4.5 +-1,0 ) x 3.0 • )• 1,41+-0.13) • 8 •

K~K-~r+ + c.c.

<

3.4

e+

<

9

2~+ 2~r4~ 0

Jf1(1285)J

10 - 3 10 - 3 10 - 5 10 - 3 • 10 - 3 • 10 - 9

IG(j PC) =

CL=9S% CL=9S% CL=90%

433.1_+ 12:1)~

s=1.3

s63

422.o_+ ]:24) ~

s=1.3

566

2~r+2~-

(11.0_+ 0:7)%

s=1.3

563

411.0_+ 017) %

S=1.3

340

CL=90%

568 479 234

4~r0 l??rlr ao(980)~r [ignoring ao(980 ) --~ Tur~r [excluding ao(980)~r ] KK'~r KK*(892) ,~p0

~7

<

7

4~

4/r 0 27r+ 27r~r+ 71"- 27r0

2(~r~r)s_wave //7/ KK ~' 3' e+ e-

J fi(1420) [n] J

~o ~o ~+ ~.-

p 09T+?r-

Full width r = 200 to 5oo MeV

Scale factor/ p Confidence level (MeV/c)

Fraction (F//F)

4,~

Mass m = 1200 to 1500 MeV (Q/r)

p (MeV/c)

0+(1 + +)

M a s s m = 1281.9 4- 0.6 MeV ( S = 1.7) Full width F = 2 4 . 0 • 1.2MeV ( S = 1.4) f1(12116) DECAY MODES

I6(jPC) = 0+(0 + +)

Scale factor/ P Confidence level 4MeV/c)

~Tr

e-

J f0(1370)[k] J

Fraction ( r i / r )

x 10 - 4

452 +-16 ) % 436 4- 7 ) % 416 4- 7 ) % ( 9.0+- 0.4)% not seen ( S.5+- 1.3)% ( 7.4+- 2.6) x 10 - 4

S=1.1

308 -

S=2.8

410

236

/G(jPC)

Mass m =1426.3 4-1.1MeV

= 0+(1 + +)

(S=1.3)

Full width F = 55.5 4- 2.9 MeV f-].(1420) DECAY MODES

Fraction ( r i / r )

KKT: f/~" 7i"

dominant dominant possibly seen

r

seen

KK'*(892) + c.c.

J ~(1420) [o] J

p (MeV/c) 439 155 571

-

I6(J Pc) = 0-(I - -)

Mass m = 1419 4- 31 MeV Full width F = 174 4- 60 MeV u(1420) DECAY MODES

Fraction (Fi/F)

p/r

dominant

p (MeV/c) 488

30

Meson SummaryTable I ~(1440) [P] I

IG(jPC) = 0+(0 -

+)

I w(1650) was ~(1600)['] I

Mass m -- 1 4 0 0 - 1470 MeV [m] Full width F =

~(1440)

DECAY MODES

Fraction seen

KK*(892) + c.c. ~TrTr ao (980) ~ 7/(Tr~r)s_wave f0 (980) ~7

seen seen seen seen

4~r

seen

I 10(1450) I

(ri/r)

p (MeV/c)

seen

Fraction seen seen

KK

seen

Fraction (ri/r)

p~ u)~ e+e -

seen

637 601 824

seen

seen

= 1-(0 + +)

~j(1670)

(r/iF)

p (MeV/c)

IG(j PC) =

0-(3 - -)

Mass m = 1667 4- 4 MeV Full width F = 168 • 10 MeV [m]

Mass m = 1474 4- 19 MeV Full width r = 265 4- 13 MeV

~ ~'(958)

1~(1650) DECAYMODES

I d3(1670) I

I6(jPC)

a0(1450) DECAY MODES

= 0-(I - - )

M a s s m = 1649 4- 24 MeV ( 5 = 2 . 3 ) Full width F = 2 2 0 4 - 3 5 M e V (S = 1.6)

50 - 80 MeV [m]

KK/r

IG(jPC)

p (MeV/c)

DECAY MODES

p~r w~r?r ~(1235)7r

p ( M eV/c)

Fraction ( r i / r ) seen seen possibly seen

647 614 359

613

392 530

IG(jPC) =

I ~r2(1670) I

1-(2 - +)

Mass m = 1670 • 20 MeV [m] I p ( 1 4 5 0 ) [q] I

IG(JPC) =

Full width F = 2 5 9 • ~r2(16"/0) DECAY MODES

Mass m = 1465 • 25 MeV [m] Full width r = 310 4- 60 MeV [m] p(1r

DECAY MODES

/r/r 47r oJTr e+ e -

P Confidencelevel (MeV/c)

Fraction ( r i / r ) seen seen <2,0 % seen <4 % not seen

~p

a2(1320)/r

~Tr

7]9 665 512 732 317

95%

3;T f2(1270) ~r pIT

95%

c.c.

p(1450)~"

b1(1235)';r

~(1680) DECAY MODES

(892) +

(rdr)

513

seen seen seen seen

690 686

I p3(1690) I

seen seen seen

737 738 563

+)

Mass m = 1525 4- 5 MeV [m] Full width r = 76 + 10 MeV [m] Fraction ( r i / r )

(08.8 .1.3.1 )%

~/T/

(10.3 ,1,3.1)%

?r~T ")'7

( 8.2 ,1,1.5 ) x 10- 3 (1.32,1,0.21) x 10- 6

IG(jPC)= 1+{3

1~j(1690) DECAY MODES

Fraction (ri/r)

4/1" ";r'• "a+ ?r-- ~ 0

(71.1 .1. 1.9 )% (67 .1.22 )%

wTr

581 531 750 763

p (MeV/c)

- -)

Massm = 16914- 5 MeV [m] Full width F= 161• MeV [m] (S=I,5)

/i'~_ p (MeV/c)

Fraction ( r i / r )

681 840 622

seen

= 0+(2 +

-)

620

4~

KK

97.7% 97,7%

seen seen not seen

T//)

DECAY MODES

x 10- 3 x 10 - 3

463

-

ft2(1525 )

453

seen

seen

IG(jPC)

% %

K}KTr

r/T/(958)

I f~(1525) I

p (MeV/c)

c.c.

K K e+ e UJ7r~r

2~ 0 KK

(4,2+1.4) (2.7• < 3.6 < 1.9

dominant

K

Fraction

/F 7r 7F+ ~r-

649

Mass m = 1680 • 20 MeV [m] Full width r = 150 • 50 MeV [m]

I6(jPC)= 0+(0 + +)

f O ( I ~ ) DECAY MODES

2~ + 27r-

806 325

IG(jPC)= 0-(1 -

541

M a s s m = 1500 4-10 MeV ( S = 1 . 3 ) Full width F = 112 • 10 MeV

4/r 0

P Confidence level (MeV/c)

(13 .1.6 ) % (8.7,1,3.4)%

cr~r fo(1370)';,r KK*(892)+ wp

Fraction ( r i / r )

1.5)

(95.8• 1.4) % (56.2 • % (31 ,1,4 ) %

358

<1.6 x 10- 3

I t0(1500) [r] I

(S=

-

<1 %

KK

11 M e V [ m ]

1+(1 - - )

KK~

KK ~'/7r+ ~ p(770) ~

(16

Scale factor

,1, 6 )%

(23.6 ,1, 1.3 )%

( 3.0 ,1, 1.2 )% ( 1.58-1- 0.26)% seen seen

1.2

P (MeV/c) 788 788 656 834 628 686 728

31

Meson SummaryTable IG(jPC)

[q] I

= 1+(1 - - )

I f2(2010) I

IG(jPC)

= 0+(2 + + )

i

Mass m = 1700 • 20 MeV [m] (F/p~ and 7r+~r - modes) Full width F = 240 • 60 MeV [m] (r/p 0 and IT+Tr- modes)

Mass m = 2011_+60 MeV Full width F = 202 • 60 MeV

~1700) DECAY MODES

Fraction (r//r)

#?lr7r pO IT+ IT-p• 7r-F,/i.0 2(IT+ 7r-)

dominant large large large

640 640 642 792

7r+ "/r-IT-- IT0

seen seen

838

K K * ( 8 9 2 ) + C.C. f/p a2(1320)Tr KK

seen

e+ e -

seen seen

IT0w

p (MeV/c)

839 479 533 692

seen

not seen seen

I ~(1710)[t] I

IG(jPC)

~(2010) DECAY MODES

Fraction ( r i / r )

a~

seen

I a4(2040)I ,14(2040) DECAY MODES

Fraction ( r i / r )

KK-

seen

IT+ I T -

662

~/IT0

IT0

Fraction (ri/r)

KK ~ ITw

seen seen seen

p (MeV/c)

IT+

I t ~T

f0 (980) I t fO ( 1 3 7 0 ) IT-

piTF/F/7rao (980) ~/

fo (1500) ITT/r/r(958) ITK~(1430) K -

1-(0

- +)

623

seen seen seen seen

459

IG(j PC) =

Mass m = 1854 • 7 MeV Full width F = R~+28 v . -23 MeV

-

728

240 -

Fraction (F;/F)

KK K K * (892) + c.c.

seen seen

0+(4 + +)

0-(3-

-)

p ( MeV/c)

785 602

Fraction (Fi/F)

p (MeV/c)

658 , 1012

ITIT

(17.0=1=1.5) %

KK

(6.8_+314) x 10- 3

895

(2.1i0.8) x 10-3 < 1.2 % seen

863 977

IG(jPC)

= 0+(2 + + )

Mass m = 2297 • 28 MeV Full width F = 149 • 40 MeV f2(2300) DECAY MODES

Fraction

(~(~

seen

I fa(2340)I

(ri/r)

IG(jPC)

p (MeV/c) 529

= 0+(2 + + )

Mass m = 2339 • 60 MeV Full width F = 319+88 MeV

560

(S = 1.2)

~3(1850) DECAY MODES

IG(JPC) =

(26 +6 ) %

p (MeV/c)

seen seen seen not seen

J

f4(20SO) DECAY MODES

I f2(2300)I

(ri/F)

seen not seen

K*(892) K J~(1850)

Fraction

892 941

w~

/'//7 4IT~ a2(1320) 7r

M a s s m = 1 8 0 1 • 13 MeV ( S = 1.9) Full width F = 210 • 15 MeV lr(1~100) DECAY MODES

p (MeV/c)

Massm=2034• ( S = 1.6) Full width F = 2 2 2 • 19 MeV ( S = 1.8)

690 648 837

i6(jPC)

1-(4 + +)

seen seen

I f4(2050) I

Massm= 1715• (S=1.1) Full width F = 125 • 12 MeV f0(1710) DECAY MODES

IG(J PC) =

Mass m = 2014 • 15 MeV Full width F = 361 • 50 MeV

850

= 0+(0 + + )

p (MeV/c)

~(2340) DECAY MODES

Fraction (o/r)

~<~

seen

p (MeV/c) 573

32

Meson SummaryTable Lepton Family number (LF), Lepton number (L), A S = ZIO (SO) violating modes, or A S = 1 weak neutral current (51) modes

STRANGEMESONS

(S=+I,C=B=O)

K + = u~,K ~

d~,~~

K - =~s,

I(J P)

r~

similarly forK*'s

= 89

Mass m = 493.677 =E 0.016 MeV [u] (S = 2.8) Mean life T = (1.2386 + 0.0024) X 10 - 8 S (S = 2.0) CT = 3.713 m Slope parameter/1" iv] (See Particle Listings for quadratic coefficients) K + --~ 7r+Tr+Tr - = - 0 . 2 1 5 4 -I- 0.0035

K-~

(S = 1.4) (S=2.5) (S = 2.7)

;T--;T--Tr+=--0.217-1-0.007

K • _~ ~ •

= 0.652 • 0.031

:r 11"+ e - Ue ~'+;T+#-~p

SQ SQ

~+ e+e -

$1

;T+,u.+,u.-

$1

Ke+3

A+ = 0.0276 • 0.0021

K+ p3

A+ = 0 . 0 3 1 •

(S=1.6)

+ K#3

Ao = 0 . 0 0 6 •

(S=1.6)

~,l, ;TO

;T'+ ;T+ ;T-;T+ ~0 ;,r0 ;T0#+U# + Called K.3. ;Toe+~e Called K+3. ;TO~0 e+ z,e

227 172

( 1.6

_+~:~) •

10-10

LF LF LF LF

< 2.0

71"-p.+ e + ;T- e + e + ir + #+~e ;T0 e + ~ e

L L L L L

x x x x x x x x x

10- 8 10- 3 10-10 10- 9 10- 9 10- 8 10- 4 10- 3 10- 3

[d] < < < < < [d] < [d] < <

4 2,1 7 7 1.0 1.5 3.3 3

I(J P)

=

227 CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% Ct=90%

236 236 214 214 214 227 172 236 228

89

mKo - mK~ = 3 . 9 9 5 • (S=1.1) ImKo _ mRol / maverage < 10-18 [bb] T-violation parameters in K ~ Asymmetry A T in K ~

~ mixing [w]

-0 mixing = (6.6 + 1.6) • 10 - 3

CPT-violation parameters in K ~ ;0 mixing [w] Re A = (2.9 -I- 2.7) • 10 - 4 Im A = ( - 0 . 8 • 3.1) • 10 - 3

1(2 P) = 89 Scale factor/ p Confidencelevel (MeV/c)

(63.51+0.18) % (1.55• x 10- 5 (21.16:h 0.14) % 5.59• % 1.73• % 3.18• %

S=1.3 S=1.1 S=1.8 S=1.2 S=1.5

236 247 205 125 133 215

(4.82•

S=1.3

228

CL=90% CL=90%

206 2O3 151 135 236

;T+ ~r- e+ Ue ~+ ~r-#+ ul~ ;TO;TO~rOe+ Ue #+ u#vP

( 2.1 • (3.91• ( 1.4 • < 3.5 < 6.0

e+ UeU~

<

#+u#e+e e+vee+e -

e+ Ue#+l~-

< <

#+ Upl~+ # -

% )x x )x x

10- 5 10- 5 10- 5 10- 6 x 10- 6

6 x 10- 5 1.3 +0.4 ) x 10- 7 3.0 +3.0 ) x 10- 8 -1.5 5 x 10- 7 4.1 x 10- 7

#+u#7 ~+ ~r~ x+;T~ ~-+;T+Ir- 7

ix,Y] ix,Y] [y,z] ix, y]

2.75• 1.8 •

It+ ~r0;T0 7

ix,y]

76 _+~:05) x 10-8

;T~

ix,Y] < 6.1 ix, Y] (2.62•

;TO;rOe+ue7 ~+77 ;T+ 37

S=3.4

Mean life ~- = (0.8935 • 0.0008) x 10 -10 s o r = 2.6786 cm

e+ u e

;T0e+ UeT(SD)

• 10- 7 ) x 10- 8

50% K s, 50% K t Mass m = 497.672 + 0.031 M e V

Fraction (Fi/F)

#+~,#

u#7

203 151

31

K - modes are charge conjugates of the modes below.

;TOe+ue7

CL=90% CL=95%

,~+,,~

F v : 0.148 • 0.010 FV < 0.23, E L = 9 0 % F v < 0.49 Fvl=-2.2to0.3

K + DECAY MODES

x 10- 8 x 10- 6

p.-- 11e"l" e "l" p.+ z:e x '+ p.+ e ;T+~-e +

K+3 Irs/r+l = 0.084 • 0.023 (S = 1.2) Ke~ (fT/r+ I = 0.38 + O . l l (S = 1.1) K p3 + IrT/r+l = 0.02 -I- 0.12 FA + K + -~ I~+U#7 I F A + K + -~ e+Ue7 F A K+ ~ #+u~7 FA-

1.2 3.0 (2.88• ( 7.6 •

r~

K • decay form factors [a,w]

K + --+ e'+Ve7

< <

5.50•

1.04•

[aa] < 6.3 < 5 [y] (1.10• [y] < 1.0

CL--90%

247 CL=90% CL=90%

• 10- 3 x 10- 4 ) x 10-5 x 10- 4

x 10- 5 x 10- 4 x 10- 5

247 236

CL=90%

x 10-6

CL=90% CL=90%

x 10- 6 x 10- 4

CL=90%

CP-violation parameters

[ccl

Im0/+_o)

= - 0 . 0 0 2 • 0.009

Im0/ooo)

= - 0 . 0 5 + 0.13

J~$ DECAY MODES

Scale factor/ p Confidencelevel (MeV/c)

Fraction ( r i / r )

~r+ ;T/r0 ;T0

7r+~r--7 7~

(68.61• % (31.39+0.28) % (1.78• • 10- 3 ( 2.4 • ) x 10- 6

[x, dd]

/r+/r--;T 0

S=1.2 S=1.2

( 3.2 +1.2 --1.0 ) x 10- 7

3;T0

<

;r•

lee]

1.4 { 7.2 •

133

x 10- 5 )xl0 -4

CL:90%

139 229

CL=90% CL=90% CL=90%

225 249 231

/ 1 5 = 1 weak neutral current (51) modes

#+lJ. 9+ e 1r e + e -

$1 S1 $1

< < <

3.2 1.4 1.1

x 10- 7 x 10- 7 x 10- 6

185

I(J P) = 89

236 205 205 125

mKL -- InKs = (0.5300 + 0.0012) x 1010 ~ S- 1

133

Mean l i f e T = ( 5 . 1 7 + 0 . 0 4 ) cr = 15.51 m

215 228 228 2o6 227 227

206 209 206 249

= (3.489 -I- 0.008) X 10 -12 MeV x 10 - 8 s

(S=

1.1)

Slope parameter lr [v) (See Particle Listings for quadratic coefficients) K o_~

;T+;T-;T0 =0.678+0.008

(S=1.5)

33 Meson

g/. decayform factors [w]

I K"(892) I

(S = 1.3)

Ke03

)~+ = 0.0288 4- 0.0015

K~

A+ = 0.034 4- 0.005

(S = 2.3)

KO 3

A0 = 0 . 0 2 5 4 - 0 . 0 0 6

(S=2.3)

Summary

Table

=

K*(892) • mass m = 891.66 + 0.26 MeV K * ( 8 9 2 ) ~ mass m = 896.10 • 0.27 M e V K * ( 8 9 2 ) • full width r = 50.8 4- 0.9 MeV K * ( 8 9 2 ) ~ full width r = 50.7 • 0.6 MeV

K,~ 1~=/41 < 0.04, CL = 68% K~~ IfT/f+l < 0.23, CL = 68% K% l~/f+l - 0.12 4- 0.12 KL -~ e+e-3': o K. = -0.33:1:0.05

(S = 1.1) P Confidence level (MeV/c)

K*(892) DECAY MODES

Fraction ( r i / r )

K~ K03'

~ 100 % ( 2,30+0.20) • 10 - 3 ( 9.9 +0.9 ) • -4 < 7 • 10 - 4

K+3'

CP-violation parameters [co]

(S = 1.4)

K~

95%

291 310 309 224

6 = (0.327 4- 0.012)%

I~ooI -- (2.262 4- 0.017) x 10 -3 In+-I = (2.270:1: 0.017) x 10-3

I K1(1270) I

I'/oo/%-I = 0.9936 4- 0.0014 ['q

~'/~ = (2.14- 0.5) x10 - 3 [ f f ] r

I(JP) = 89

Mass m = 1273 4- 7 MeV [m]

(S = 1.6)

Full width r = 90 :I: 20 MeV [m]

i S--1.6)

= (43.3 4- 0.5) ~

~oo = (43.2 + 1.0) ~ ~oo - ~ + - = ( - o . 1 4- 0.8) ~ CP asymmetry A in KL0 -~ l r + T r - e + e - = (13.6 • 2.8)% ] f o r K [ --* Ir+Tr- 7r0 = 0.0011 4- 0.0008

K1(1270 ) DECAY MODES

Fraction ( r i / r )

Kp K~i1430)Tr K*(892)~r

442 4-6 ) % (28 • )% 416 +5 ) %

K~ K f0(1370)

(11.0• % (3.0+2.0) %

p (MeV/c) 76

301

f f o r K ~ -~ ~+~r-Tr ~ "= 0.004 4- 0.006

I~+-~I-- (2.35 4- oo7) x lO-3

I K1(1400) I

~ + - 7 = (44 4- 4) ~ J

Ic+_=l/e < o.3, CL = 90%

Full width r =

decay Re x = - 0.002 • 0.006

AS = - A O in ~

Im x = 0.0012 4- 0.0019 K0L DECAY MODES

Scale factor/ p Confidence level (MeV/c)

Fraction ( r i / r )

370 ~+/r-Tr 0 7r'l-#~:up

421.13 +0.27 ) % (12.55 • )% (27.18 +0,25 ) %

[ee]

S=1.1 S:1.7 5=1.1

139 133 216

174 4- 1 3 M e V

[ee]

~+e~FUe Called Ke~ . 23' 33' 7023' ~0x+eTp /lr#atom)u

(38.78 +0.28 ) %

( 5.06 < 2.4 [gg] ( 1.68 [ee] ( 5.18 ( 1.o6

[x, ee,gg]

229

10 - 4 10 - 7 CL=90% 10- 6 10- 5 10- 7

249 249 231 207 -

( 3,62 +0.26 --0.21 ) • 10--3

~+~..3'

(57

"K+ ":,r--3" ~0Ti'03' /z+/4-3' e+ e-3' e+e-3'3' ;T~ + e -

+0.15 ) x x • )x +0,29 ) x +0.11 ) x

5=1.1

[x,gg]

( 4.61 < 5.6 ( 3.25 410,0 [gg] 46.9 < 7,1

+~:~

)•

229

(S=

1.6)

/(1(1400 ) DECAY MODES

Fraction ( r i / r )

p (MeV/c)

K*(892)~r Kp K fo(1370)

(94 • )% (3.0• % (2.0• % 4 1.0+1.0) % not seen

401 298

K~ K~(1430)~r

205

i

I(J P) = 89

I K*(1410) I

Called K~ .

lr~'em Ve3"

I(JP) = 89

Mass rn = 1402 4- 7 MeV

( S = 1.3)

Massm=1414• 15 M e V Full width F = 2 3 2 •

(S=

1.1)

K*(1410) DECAY MODES

Fraction ( r / / r )

K*(892)~r

> 40 (6.6• < 7

K~r Kp

P Confidence level (MeV/c)

% % %

95% 95%

408 611 309

-

+0,14 ) x 10- 5 • 10- 6 +0.28 ) x 10- 7 • ) x 10- 6 S=1.5 +1.0 ) x l 0 - 7 x 10- 7 Ct=90%

206 209 225 249 249

Charge conjugation x Parity (CP, CPV) or Lepton Family number (LF)

I K~(1430) ~] I

I(JP) = 89176

Mass m -- 1412 4- 6 MeV Full width r -- 294 4- 23 M e V

(ri/r)

K~(1430) DECAY MODES

Fraction

K/r

(93+10) %

p (MeV/c) 621

violating modes, or ~S = 1 weak neutral current ($I) modes lr+Tr 1r0;r 0 #+#-

CPV CPV $1

(2.056+0.033) x 10- 3 ( 9.27 • ) x 10- 4 ( 7,15 • ) x 10- 9

206 209 225

e+ e-

S1

( 9

Jr 46

) x 10 -12

249

( 3.5

+0.6

) x 10- 7

206

(2.9

+_~]7 ) x l O - - 9

225

( 4.1 5.1 4,3 5.9 4.7 6.1 6.2

+0,8

249 177 231 231 238 -

7r+Tr-e+e -

51

#+#-e+e

S,Z

-

e+e-e+e "KOt~+Ir T~ ~rOu~ e+/J. ~

e+ e+ #=l.~R= x~

m

[gg]

51 CP,S1[hh] CP,SI[hh] CP,SI [fi] LF [ee] LF [eel LF [ee]

< < < < < <

)x x x x x x x

10- 8 S=1.2 10 - 9 CL=90% 10 - 9 CL=90% 10 - 7 CL=90% 10-12CL=90% 10- 9 CL=90% 10- 9 CL=90%

I K;(1430) I

I(JP) = 89

K~(1430) "~ mass m -- 1425.6 4- 1.5 M e V (S -- 1.1) K.~(1430) 0 mass m -- 1432.4 4- 1.3 M e V K~(1430) + full width r = 98.5 • 2,7 M e V (S = 1.1) K~(1430) ~ full width r -- 109 4- 5 M e V (S -- 1.9) K~(1430) DECAY MODES K/r K * (892) '/r K*(892)~rlr Kp

Fraction ( r i / r ) 449.9+1.2) % 424,7 • 13) % 413.4+2.2) % (8.7• %

Scale factor/ p Confidence level (MeV/c)

S=1.2

622 423 375 331

34

Meson Summary Table Kw K+7

(2.9--0.8) % (2.4:50.5) xlO -3

S=1.1

319 627

KT/

(1.5+314) x 10-3

S=1.3

492

CL=95% CL=90%

110 631

K~r K~

< 7.2 < 9

I K*(1680)I Massm= 1717• Full width F = 3 2 2 •

x 10-4 x lO-4

II

CHARMEDMESONS

(c= +z)

D + = cd, D o = c~, ~ o = ~u, D - = ~d,

similarly for D*'s

I(J P) = {(0-)

I(JP) 89 =

Mass m = 1869.3• MeV ( S = 1 . 1 ) Mean life 7" = (1.051 • 0.013) x 10 -12 s cr = 315 pm

( S = 1.4) 110MeV ( S = 4 . 2 )

K*(1680) DECAY MODES

Fraction ( r i / r )

p ( MeV/c)

K~r

(38.7--2.5) %

779

Kp

(31.4-+24h7) %

571

K*(892) ~r

(29.9-+2:~) %

615

I K2(1770)[kk] I

c-quark decays r ( c --~

D + ---, K * ( 8 9 2 ) ~

Mass m = 1773 • 8 MeV Full width F = 186 • 14 MeV Fraction ( r i / r )

K?TTr K~ (1430) 7r K* (892) ~ K f2(1270 ) K~ K~

dominant seen seen seen seen

anything) = 0.095 • 0,009

[ram]

Acp(K + K - 7r--) = - 0,017 + 0.027 Acp(K • K *~ = - 0 . 0 2 • 0.05 Acp(@Tr--) = -0.014 • 0.033 Acp(~+~:-~: • = -0.02 • 0.04

;(JP) = {(2-)

E2(1770) DECAY MODES

@+anything)/r(c -~

CP-violation decay-rate asymmetries

form factors

rv =

1.82 • 0.09 r2 = 0.78 • 0.07 r3 = 0.0 • 0.4 FL/F T = 1.14 • 0.08 r+/r_ = 0.21 • 0.04

p (MeV/c) 287 653 441 608

(S = 1.3)

D - modes are charge conjugates of the modes below. D+ DECAY MODES

Scale factor/ p Confidencelevel (MeV/c)

Fraction ( r i / r )

Inclusive modes l(J P) = { ( 3 - )

I K;(1780) I M a s s m = 1776• 7 MeV Full width F = 1 5 9 •

( S = 1.1) (S=1.3)

K~(17ao) DECAY MODES

Fraction ( r l / r )

Kp

(31 "- 9 ) % (20 • 5 )% (18.0-- 1.0) % (30 --13 )% < 16 %

K*(892)Tr K~r KT/ K~(1430) 7r

I

K2(1820)["]1

e+anything K-anything K~ + K+ anything ~/ anything

95~

Fraction ( r i / r )

K,~(1430) 7r K* (892) 7r K f2(1270) Kc~

seen seen seen seen

I K~,(2045) I

p (MeV/c) 325 680 186 638

KTr K*(892)lrlr K*(892)~r~Tr

(9.9 • % (9 • )% (7 /:5 )% (5.7 • 3.2) % (5.0• % (2.8'-1.4) % (1.4"-ox) %

pKx wK~ ~K~@K*(892)

K-/r + e+ v e

K*(892)~ x B(K *0--~ K - ~ +) K-Tr+l~+U~, nonresonant (K*(892) 7r)0 e+ Ue (KlrTr)~

K-Tr+TrO#+up "KO~+Pl

K-*(892)~ K*(892) 0 e+ ue K*(892)0#+u# K1(1270)~ v#

M a s s m - - 2045+ 9 MeV ( 5 = 1.1) Full width r = 198 • 30 MeV Fraction (Fi/F)

Ve

e+

~0/i,+ U~,

932

[oo] (6.0:5 0.8 )% (6.7 • 0.9 )% ( 7.0 + 3.0 )% - 2.0 ( 4.1 + 0.9 )% - 0.7 ( 3.2:5 0.33)% < 7 x 10-3 ( 3.2 • 0.4 )% ( 2.9:5 0.4 )% ( 2.7 -- 1.1 < 1.2 < 9 < 1.4 [pp] ( 3.1 • 1.5

)xlO -3 % x l 0 -3 x 10-3 ) x l 0 -3

B08 865 863 720 CL=90% S=1.1

CL=90% CL=90% CL=90%

863 851 715 851 714 846 825 930

Fractions of some of the following modes with resonanceshave already appeared above as submodes of particular charged-particlemodes.

I(JP) = {(4+)

K~(2045) DECAY MODES

CL=90%

( 8 --+17 ) x 10-4

~+ ~ ~ t+ vt

K-x+l~+Up

Mass m = 1816 • 13 MeV Full width r = 276 • 35 MeV

S=1,4

Leptonic and semileptonic modes

K * (892) 0 e+ v e x B(K*~ K - T r +) K - ~ r + e+ v e nonresonant

I(JP) = 89

K2(11120} DECAY MODES

K~

p Confidencelevel (MeV/c) 612 6,51 810 71s 284

(17.2 • 1.9 )% (24.2 • 2.8 )% (s9 :5 7 ) % ( 5.8 • 1.4 )% [nn} < 13 %

p ( MeV/c) 958 800 764 742 736 591 363

K*(1410)O#+vp K'~(1430)~

pOe+ue p0/~+p/~

~e+Ue (~JJ,+U# ~7~+tll r/'(958)#+u#

[oo]

( 4.7 i 0.4 )% ( 4.8 • 03 ) % ( 4,4:5 0.6 )% < 3.5 % < 2.7 % < 8 xlO -3 ( 2.2 • 0.8 } x l 0 -3 ( 2.7 • 0.7 ) x l 0 -3 < 2.09 % < 3.72 % < 5 x l 0 -3 < 9 x l 0 -3

S=l.l CL=95% CL=95% CL=95%

CL=90% CL=90% CL~90% CL=90%

720 715 493 389 374 776 772 657 651 684

35

Meson Summary Table Hadronic modes with a K or K K K K - ~+ ;T+

2.894. 0.26) % 9.0 4- 0.6 ) % 1.27• 0,13) %

[qq]

K * (892) 0/r + x B ( K *0 --* K - ~ r + ) K~ (1430)~ +

x B(K*(1430) ~

S=1.1

2.3 4- 0.3 )%

862 845 712 368

K-;T +) 3.7 4- 0.8 ) x 10- 3

g*(1680)~ ~r+ x B(g*(iB80)O--~ K-;T 4") K - ~r4"7r4" nonresonant

"~0 ;T+ ,RO

8.5 • 0.8 )%

[qq]

9.7 4- 3.0 )% 6.6 4. 2.5 )% 6.3 • 0.4 )x 10- 3

~0 p+ K * (892) 0 ~r+ x B(g*0 -~ K%r 0) ~+ ~r~ nonresonant

K - ~r+ ;T+ ;TO

65

5=1.1

845 816 423

1,3 4- 1.1 )% 6.4 4- 1.1 ) %

[qq]

845 845 680 712

K ~ ( 1 4 3 0 ) 0 ;T+

3.7 •

0.4 )%

368

K*(1680)%r + g * (892)0 ;T+ ;T0 total ~ ' , (892)0 ~ + ;To 3-body K * ( 8 9 2 ) - ;T+ ~r+ 3-body K - p+ ;T+ total K - p+ 7r+ 3-body ~ o po ;T+ total ~OpO ;T+ 3-body

1.43• 6.7 • 4.2 • 2+0 • 3.1 • 1.1 ~ 4.2 • 5 • 5

0.30) % 1.4 )% 1.4 )% 0.9 )% 1.1% 0.4 %

65 687 687 688 616 616 614 614 461 642

[-]

go fo (98o) ;T+ K * (892) 0 ;T+ ;T+ ~r-

<

4- 3.4

% x 10- 3 x 10- 3 x 10- 3

( 2.9 4- 1.7 -- 1.5 ( 4.3 4- 1.7 ( 3.1 4- 0.9

x 10- 3 x 10 -3

(8.1

~ * (892)0 pO ~ +

K * ( 8 9 2 ) 0 ~ + ;T+ ~r- no-p K-pO;r+Tr +

0,9 5

x 10- 3

1.4 4- 0.9 ) %

K1(1400)0 ;T+ x B(KI(1400)0--~ K - ; T + " a 0 )

2.2 4- 0.6 ) %

390

K- p+ ~r+ total K- p+ ;T+3-body

3.1 • 1.1 • 4.5 •

1.1 )% 0.4 )% 0.9 )%

616 616 687

;T+ ?r4"/r- 7r0

2.8 •

0.9 )%

687

~ r + 7r+ 7r+ ~ r - ;T -

6.9 4- 1.4 ) x 10- 4 6 x 10- 3 2.1 4- 0.4 ) x 10- 3

;T+/r+ ;T+ ;T- 7r- 7r0

2.9 4- 2.9 ) x 10- 3

~o ~+ ;T+ ~r-

;T+ ; T + x -

7 [rr]

::t= 3

)xl0 -3

po;T+ ~r+ ~r+ ;T- nonresonant

'q;T+ x B(r/--, :,r+;T-;T ~ w-a-+ x B(~ --, 7r+;T-;T ~

816 814 328

2.2 4- 0,6 )%

390

~p4,

K * ( 8 9 2 ) - ;T+ ~r+ 3-body x B ( K * - -~ ~ O ; T - ) n o pO ;T+ total ~ o pO ~r+ 3-body ~ o ~r+ ;T+ ;T- nonresonant

1.4 •

688

7/(958)7r + r/(958)p +

0.9 ) %

0.6 ) %

119 ~

~:)) %

10- 3 10- 3 10- 3 10- 3

925 908 769 908

882 CL=90%

B48 764 845 799

2,0

10- 3 10- 3 10- 3 10- 3 10- 3 10- 3

CL=90% CL=90% CL=90%

848 769 764 658 680 355

5 8 7.2 5.4

K - ;T+ ~r+ ~ + ;T- nonresonant

5 4 1,0 2,3

x x x x

614 814 712 642

10- 3 10- 3 10- 3 10- 3

( 1.9 4- 1.1 - 1.0

x 10- 3

242

( 2.9 4- 1.1

x 10- 3

642

( 3.1 4- 0.9 < 2.3

x 10- 3 x 10- 3

K-;T +)

"K* (892) 0 ;T+ ;T+ ;T- no- p x B ( K *0 --* K - ; T + ) K-p0;T+;T +

• 44•

Hadronic modes with a K K pair

614

4.2 4- o.9)%

~ * (892)0 po ~r+

CL=90%

K4"K0

( 7.4 •

K 4" K - ;T+ q~'/r+ X B(~b ~ K+g*(892) 0

K + K-)

x B(K *0-~

K - ~ +) ( 4.5 • 0,9 ) x 10- 3

K*(892)+K0 x B(K *+-~ K + K - ;T+ ;T0

( 2.1 •

~r+;T0 x B(~--* K+K - ) ~p4" X B(@-~ K+K -)

775

K + K - ;T+ ;TOnon-r

g o ;T+ ;T4. ;T- ;TO

5.4 + 3.0 - 1.4 8 • 7 2.0 • 1.8 1.8 • 0.8

%

773

K + ~O,K+,lr -

10- 4 x 10- 3 %

714

K~

~o ~o K +

718 548

gOp+

( 6.6 4- 2,5 ) % ( 8.o 4- 1.7 )% < 3 x 10- 3

K~ K~

K*(892)0;T +

CL=90%

( 1.9o4- o,19) %

[rr] [rr]

( 2.1 4- 1.3 ( 1,6 + 1.6

< I (lO <

7

4- 7

% % x 10- 3 x 10- 3 x 10- 3

x 10- 3 7 ( 4.9 4- 1 . 2 ) % < 7 x 10- 3 <

CL-90% CL=90% CL=90% CL=90%

680 328 199 712 423 423 423 423 423 407 390 382

1.o )%

(1.1• EL=90%

<

CL=90%

678 678 273

-

K*(892)4"'/~*(892) ~ x B 2 ( K * + -~ K 0 / r + )

q~Tr+ 7r4-/rx B(r

2

682

0.6

%

( 1.0 4- 0.6 )% ( 1.2 •

*~

K +K-) K+K-Tr+Tr+~r-nonresonant

682 619 268

< 7 xl0 -3 ( 1.5 + 0.7 ) %

+

K~ K+ K - ~ + ~ r + ~ -

Fractions of some of the following modes with resonances have already appeared above as submodes of particular charged-particle modes.

744 741 611

KO;T+)

529 772

%

X

792 744 647 610

( 3,0 4- 0,3 ) x 10 -3 ( 2.8 • 0.4 ) x 10- 3

K + K - ~r+ nonresonant KO~O~+

2.2 4, 5.0 - 0.9

K ~ ;T+ 7r4"7[+ ;T ;T K - ;T+;T+ ;T+ ;T- ~ro

1.0 ) x 10- 3

[qq] ( 8.7 • 0.7 ) x 10- 3

K - ;T+ ;T+ ;T%r0

K * ( 8 9 2 ) ~ + D-wave Iongitudinal K1(1270)0 ;T+ K1(1400)0 ;T+ K*(141O)0;T +

642 529

D

[qq]

K*(892)~ + P-wave K*(892) 0 p+ D-wave

0.7 ) x 0.4 ) x 0.31) x 0.4 ) x

( 3.0 • 0.6 ) x ( 1.05• 0.31) x < 7 x < 7 x ( 5.0 • 1.0 ) x < 5 x

pOlr+ u,';T+

K * (892) 0 ~ + ~r+ ;Tx B(K *~ K-;T +)

K*(892)~ g * (892)0 p+ 5-wave

2,5 43.6 41.0542.2 •

-

r/';T-'-

4.0 •

x B(K * ~

242

Fractions of some of the following modes with resonances have already appeared above as submodes of particular charged-particle modes.

g o a1(1260)+ x B(a1(1260)+ -~ ;T+;T+;T-) K1(1400) 0 ~r+ x B(K'1(1400) 0 - ~ g O ; T + ; T - )

K - ;T+ ;T+ ;T+ ~r-

5--1.8

688

1.2 4- 0,6 ) % 7.0 4- 0.9 ) %

[qq]

CL=90% 5=1.7

Plonlc modes 'a"+ ;T0

K * (B92)0 p+ total x B(K *0-~ K-~ +)

~ * (892)0 ;T+ ;TOtotal x B ( K *~ - * K - ~ ' + ) K * (892) 0 ~r+ ~r~ 3-body x B ( g *~ -~ K - ;T+) K * ( 8 9 2 ) - ~r+ ;T+ 3-body x B ( K * - -~ K - ; T 0) K - ;T+ ;T+ ~r~ nonresonant

CL-90%

0,5 )%

<

73

xlO -3

CL=90%

<

1

x 10- 3

EL=90%

678 600 565

<

3

%

EL-90%

600

Fractions of the following modes with resonances have already appeared above as submodes of particular charged-particle modes. ~;T+ ~;T4-?r 0 (~p+ (~T+;T4";T -

K+~*(892) ~ K*(892)+K ~ K*(892)+K*(892) ~

( 6.1 • ( 2.3 • < 1.4 < 2

0,6 ) x 10- 3 1.0 ) % % X 10- 3

CL=90% CL=90%

647 619 268 565

( 4.2 • 0.8 )• 10-3

61o

( 3.2 • ( 2.6 •

611 273

1.5 )% 1.1 )%

36

Meson SummaryTable Doubly Cabibbo suppressed (DC) modes, A C = 1 w e a k neutral current (C1) modes, or Lepton Family number (LF) or Lepton number (L) violating modes K+/r+/r DC ( 6.8 • 1.5 ) x 10 -4 K+p 0 OC ( 2.5 • 1.2 ) x 10- 4 K*(892)~ + DC ( 3.6 • 1.6 ) X 10- 4 K+~r+/r-nonresonant DC ( 2.4 • 1.2 ) x l 0 - 4 K + K + KDC < 1.4 x 10- 4 CL=90% (~K + DC < 1.3 x 10- 4 CL=90% ~r+ e + e C1 < 5.2 x 10- 5 CL=90% "/r+ # + # C1 < 1.5 x 10- 5 EL:90% p+#+#CI < 5.6 x 10 -4 CL=90% K + e+ e [s5] < 2.0 x 10 - 4 CL=90% K+#+# [ss] < 4.4 x 10- 5 CL=90% 7r+ e• :tLF [eeI < 3.4 x 10- 5 CL=90% K + e• LF [ee] < 6,8 x 10- 5 CL=90% ~r- e + e + L < 9.6 x 10- 5 CL=90% ~r-#+#+ L < 1.7 x 10- 5 EL=90% 7"('- e + # + L < 5.0 x 10 -5 CL=90% p-#+#+ L < 5,6 x 10- 4 CL=90% K- e+ e+ i < 1.2 x 10- 4 CL=90% K-/~+# + L < 1.2 x 10- 4 CL=90% K - e+ # + L < 1.3 x 10 - 4 CL=90% K*(892)-#+# + L < 8.5 x 10- 4 CL=90%

Hadronic modes with a K or ~ K K K - ~T+ ~ 0 ~0 845 681 712 845

550 527 929 917 759 869 856 926 866 929 917 926 759 869 856 866 703

l(J P) = 89

Massm-- 1864.5+0.5 MeV ( S = 1.1) roD• - mDo = 4.79+ 0.10 MeV (S = 1.1) Mean life ~- = (0.4126 • 0.0028) • 10-12 s cr = 123.7 #m

Imoo -

mDo ]

<

7 • 1010 ~. s- 1 , CL = 9 5 % [it]

(ro• - roo)Iroo: -0.116 < a r l r < 0.020, CL = 95% [tt] F(K+s

(via D ~

< 0.005, CL = 90%

F(K+~r-(via ~~

< 4.1 x 10 -4, CL = 95%

CP-violation decay-rate asymmetries

Acp(K + K - ) = 0.026 :E 0.035 Adp(/r+Tr -) = -0.05 9 0.08

Acp(K~

= -0.03 -4- 0.09

Acp(K~176) = - 0 . 0 1 8 ~E 0.030 Acp(K=~r ~) = 0.02 + 0.20

D O DECAY MODES

e+anything #+anything K - anything K~ +

K~

Indudve m o d e s (6.75/:0.29) % ( 6.6 • )% (53 • )% (42 /:5 ) %

K+anything ~/ anything

( 3.4 +~

[nnl < 13

S=1.3

)% %

--

CL=90%

-

[ooJ (3.47• (3.64• (3,22•

% % %

S=1.3

867 867 863

K-~rOe+ue

( 1.5 +~:53 )%

061

~~

( 20 _+~:~ )~

9oo

K * ( 8 9 2 ) - e+ ue X B(K*- -* K~ K - :r :r # + //# (K*(892)/r)-#+u,

(1.35/:0.22) %

719

~r-e+~e

<

1,2 < 1.4 ( 3.7 •

x 10- 3

x 10-3

CL=90%

CL=90%

)xl0 -3

821 693 927

A fraction of the following resonance mode has already appeared above as a submode of a charged-particle mode. K * ( 8 9 2 ) - e+ ue

( 3.0 •

~-0 f2 (1270) x B ( f2 --* ~ + T r - ) ~ o fo (1370) x B ( f0 ~ 7r+Ir- )

( 2.4 /:0.9

x 10- 3

( 4.3 •

x 10- 3

K*(892)-~T + x B(K*- --~ ~0/r-)

( 3.4 •

%

(2.02/:0.33) %

{qq]

( 5.4 •

(1.21•

861 860 842

676 549 263

711

x 10- 3 ( 6.4 /:1,6 K~(1430)- 7r+ x B(K~(1430)- -~. K 0 1 r - ) K'0 ~r+ 7r- nonresonant (1.47/:0.24) % K-Tr+~O [qq] (13.9 +0.9 )% (10.8 + 1 . 0 )% K-p+ ( 1.7 • )% K * ( 8 9 2 ) - 7r+ x B ( K * - -~ K - / r 0 ) ~*(892)o/rO ( 2.1 • )% x B(K *0 --, K - / r +) ( 6.9 • ) • lO- 3 K - ~r+ Tr~ nonresonant KO 7tO;r0 K*(S92)0/r 0 ( 1.1 • )% x B(K*O--* K~176 ?.g /:2.0 ) • 10- 3 K-~ 7r0 ~r0 nonresonant K-Tr+ x+ ~r[qq] 7.49• % K - 7r+ po total 6.3 /:0.4 ) % 4,7 • ) • 10 - 3 K - x + pO 3-body K*(892)~ 0 9,8 • ) x 10- 3 x B ( K * 0 - ~ K - / r +) 3.6 • )% K - a1(1260)+ x B(al(1260) + -, /r+Tr+/r -) K*(892) 0/r + ~ - total 1.5 /:0.4 )% x B(K*0-~ K-/r +) 9.5 • ) • lO - 3 K * (892) 0 / r + / r - 3-body x B('K *0 -~ K - / r +) 3.6 • ) • lO - 3 K 1(1270)- 7r+ [rr] x B ( K l ( 1 2 7 0 ) - - * K-Tr+~r - ) K - 7r+ 7r+/r- nonresonant 1.74• % KO ~ + / r - 7tO [w] (1o.o • )% KOT/ x B@/-~ ~r+x-~r 0) 1,6 • ) • 10- 3

K'(B92)~ 0 x B ( ~ *~ -* ~ % o )

[rr] K 1 (1270)-/r + x B ( K l ( 1 2 7 0 ) - - , K'~176 K*(892) ~ + ~r- 3-body x B(K*0 -~ K 0 / r ~ -~0 ~r+ ~r-/r ~ non resonant K - ~r+ ~r~ ~o K - ~r+ ~r+ ~r- ~ro

~* (892) 0/r + ~rx B(K *0--,

Semileptonic modes

K-s K-e+ue K-#+IJIj

~o fo(980) x B ( f0 --* /r+Tr-)

K0 ;T+/r~-0p0

S=l.1 S=1.2

1.9 -I-0.4 ) % 4.1 • )%

364

S=1.3

842 844

678 711 709 844 843 709 843 812 612 612 418

327 683 603 483 812

812 772 670 422

x B ( K * - -~ ~ o ~ - ) Scale factor/ p Confidencelevel (MeV/c)

Fraction (Fi/F)

%

(2.11•

% % % x 10- 3

# ~ x B(~ -~ ~+~-Tr ~ K*(892)- p+

~0 modes are charge conjugates of the modes below.

(3.83•

719

;TO

) • 10- 3

418

5.1 •

) X 10- 3

483

4.8 4-1.1 ) • 10-3

683

2.1 • (15 •

)% )%

812

4.0 •

)%

1.2 •

)%

815 771 641

2.9 •

) • lO - 3

580

2,7 • 7 •

)% ) • 10- 3

605 406

( 5.8 •

) • 10 - 3

768

(10.6 +7.3 -3.0 ( 9.4 • ( 4.3 • ( 5.1 • ( 8,3 •

)%

771

) x )• ) • ) x

( 2.1 •

) x 10 - 4

K - ~ +)

g*(892)0~/ x B(K *0-~ K-/r +) x B(~/-~ ~r+~r-~r O) K--~T+U~ X B(u~ --+ / r + x - / r 0) -K* (892)~ up x B ( K .0 ---* K - ~r+) x B(o.'--, 7r+~r-~r0) 'K'O ~+ x + / r - ~ ~ 0 ~-+ ~ - ~0/tO (~0)

~OK+ K ~OCx B(~--* K + K -) ~ o K + K - non-~ KO k,O ~0

5"S"S K+ K - K-~r + K + K - ~%r o

4.9 •

10 - 3 10 -3 10 - 3 10 - 4

( z2 -+~i~ )• lO-3

544

520 544 538 434

435

37

Meson Summ ary Ta ble KS,~S,, O~-o . o

Fractions of many of the following modes with resonances have already appeared above as submodes of particular charged-particle modes. (Modes for which there are only upper limits and K*(892) p submodes only appear below.) ~ o pO

K-p+

~o ~,(958) ~ o fo (980)

~o~

K - a1(1260) + ~ 0 a1(1260) ~ -~o f2(1270) K - 82(1320) + K ~ fo(1370) K * ( 8 9 2 ) - ~r+

R* (892)0 ~r~ K * (892) ~ ~r+ ~r- total K * (892) 0 ~r+ ~r- 3-body K - ~r+ pO total K - ~r+ pO 3-body K*(892)~ 0 ~ * ( 8 9 2 ) o po transverse ~ , (892)0 pO S-wave ~ , (892)0 pO 5-wave long. ~ , (892)0 pO P-wave ~ , (892)0 pO D-wave K * ( 8 9 2 ) - p+ K * ( 8 9 2 ) - p+ longitudinal K * ( 8 9 2 ) - p+ transverse K * ( 8 9 2 ) - p+ P-wave K - ~ + f0(980) K * (892) 0 f0 (980) K 1 ( 1 2 7 0 ) - ~r+ K 1 ( 1 4 0 0 ) - ~r+ KI (1400) 0 ~r~ K * ( 1 4 1 0 ) - ~+ K ~ ( 1 4 3 0 ) - ~r+ K ~ ( 1 4 3 0 ) - ~r+ R~(1430)0 ~0

) x 10- 3 % )%

( 2.1 •

)%

670

% ) x 10- 3 ) x lO - 3 )% % ) x 10- 3 x 10- 3 ) x 10- 3 )% )% )% % )% ) x 10- 3 % )% )% x 10- 3 x 10- 3 )% )% )% )% % % • 10- 3 % % % % % • 10- 3

565 549 520 327 322 263 197

4

x 10. 3

( 1.8 •

)%

( 1.9 • ( 3.0 • ( 1.1 •

)%

)% )% ( 7.0 ~-1.8 ) • 10- 3 < 1.0 x 10- 3

Pionic modes 1.52• 8.4 -t-2.2 16 • 7.3 • 1.9 • 4.0 •

~T-t-~rwO'/FO ~+;r--;r 0

~r+~r+~r-~'w• 0 ~r+~T+~T+7~ /r 71"

r

( 7.0 • (1.21• (10.8 • (1.71• ( 5.7 • ( 8.6 • ( 7.3 • < 1.9 ( 4.1 • < 2 6.9 • 5.0 • 3.1 • 2.2 • 1.42• 6.3 • 4.7 • 1.46• 1,5 • 2,8 • < 3 < 3 ( 1.9 • ( 6.1 • ( 2.9 • ( 3,2 • < 1.5 < 1.1 < 7 [rr] (1.06• < 12 < 3.7 < 1.2 (1.04• < 8 <

K * ( 8 9 2 ) 0 ~r+ ~r- ~r0 ~ * (892) 07/ K - ~r+~: K*(892)~ K - ~r+ fi'(958) K * (892)~ q'(958)

K+K-~+~

• 10- 3 ) • 10- 4 )% ) • 10- 3 )% )xl0 -4

S=1.2

CL=90% CL:90% 5:1.2

772 676 678

~ 0 K + ~r-nonresonant

K+K-~r ~

x B(r

cpO x B ( r K+K-p~ K*(892)~

K+K -) K+K -)

• B(K *0-~ K+~ -) K*(892)OK*(892) 0 X B2(K*0-* K+~r -) K + K - ~r+~r- non-~b K + K - ~ + ~r- nonresonant KOK0"/r+?r -

( 6

<

K+K-~r+~r-~r ~

<

K*(892)0K 0 K*(892)-K + ~;r 0 ~T/ (~0J (~/r+ ~r-

<

CL=90% CL=90%

K + ~r- 7r+ ~ -

CL=90%

641 580 505 406 479 99

CL:90% CL:90% CL=90% CL=90% CL:90% CL:90%

S=2.7

K+Tr-Tr+~-(viaD ~ K+Tr-or K + 7r- 7r+ ~r- (via 9 0 ) # - a n y t h i n g (via 9 ~

C2M DC

C2M DC C2M

C1 CI

791 788 739 605

o) e+ eo)p,'}-~ ~e + e ~p,+ p,e+ e I~+/J,-

C1 C1 C1 C1

K * ( 8 9 2 ) 0 e+ e K*(892)~ -

) x 10- 3 )xlO -3 • 10- 4

739 739 605

( 1.2 •

) x 10- 3

610

( 3.8 + 2.3 ) x 10- 3 -1.9 ( 1.3 • ) • 10- 3

739

CL=90%

K + t - P t ( v i a 9 0) K + ~K + 7r- (via 9 ~

C1

( 2.3 • ( 5.o • < 5

742

257

CL=90%

676 676 673 600

•

x 10-3 ) x 10-3

CL=90%

605 610

• }x • • • x

CL=90%

605 610 644 489 239 614

10- 4 10- 3 10- 3 10- 3 10- 3 10- 3

modes 2.4 2.4 1.9 7.6

CL=90% CL=90% CL=90%

260

)•

• x x •

10- 4 10- 4 10- 4 10- 4

CL=90%

614 257

CL=90% CL=90% CL=90% CL=90%

773 768 654 717

Doubly Cabibbo suppressed(DC) modes, AC = 2 focbiddenvia mixing (C2M) modes. AC = 1 weak neutral current (C1) modes, or Lepton Family number (LF) violating modes

p0 e § e p0/~+/j-

610

1.6 ( 3.5 •

Radiative < < < <

p0,}, ~"7 ~7 K*(892)0~

TI~+I~-

) x lO - 3

• 10- 4 ) x 10- 3 )xlO -3

( 7 • ) • 10- 4 [vv] < 7 x 10- 4 ( 1~4 - 0 . 5 ) x 10- 3

C1 C1 C1

( 2.3 •

8 ( 6.8 • ( 3.1 •

(6

~Tr + ~ - 3-body K*(O92)~ - c.c. K*(892)~ 0

~r0 e + e ~.0/~+/~T/e+e -

x 10- 3 ) x 10 - 4 )xl0 -3 x lO- 3

5=1.2 S=1.1 CL=90%

~po

C2M C1 C1

(4.25• ( 6.5 • ( 6.4 • < 1.1

) • 10- 4

8 ( 1.8 • < 1.4 < 2.8 < 2,1 (1.07•

e+ e IZ+p, -

922 922 907 879 844 795

•

Fractions of most of the following modes with resonances have already appeared above as submodes of particular charged-particle modes.

K*(892) ~ 0 K*(892) + K -

Hadronic modeswith a K~' pair K + KK0K O KOK-~r + K*(892) 0K 0 x B ( K * 0 - ~ K - ~ r +) K*(892)+K x B(K *+--, K%r +) K~ KOK+~rK*(892)0K 0 x B ( K *0 --~ K + ~ r - ) K*(892)- K + x B ( K * - -~ ~ o v - )

5.9 xl0 -4 ( 2.50•215 -3 (5.3 • -4 ( 3.0 • )xl0 -4 ( 9.0 • ) x 10- 4 [w] < 5 x 10- 4

[uu]

711 709 603 683 612 612 418 418 418 418 418 418 422 422 422 422 459 403 386 387 378 364 367 363

CL:90% CL:90%

739 676 614 260 309 528

<

-

9It + 7r--'K0 I~+ p-p+ e~ 7r~177 ~ ~e • i~:F ,o0 @• ~Twe • ~ : ~e • i~:F -~0 e-F ~ : K * ( 8 9 2 ) ~ 1 7 7 :F

C1 LF LF LF LF LF LF LF LF

<

1.7 (1.46• < 1.6 ( 1.9 • < 4 < 1.0 < 4 < 6.2 < 4.1 < 4.5 < 1.8 < 1.1 < 5.3 < 1.0 < 2.3 < 1.8 < 8.3 < 5.2 < 4.1 [ss] < 1.1 [ss] < 2.6 [ss] < 1.4 [ss] < 1.18 < 8.1 [ee] < 8.1 lee] < 8.6 [eel < 1.0 [eel < 4.9 lee] < 1.2 lee] < 3.4 [eeI < 1.0 [ee] < 1.0

x 10- 4 x 10- 4 x 10- 5 ) x 10- 4 xl0 -4 x 10- 3

CL=90%

CL=90% CL=90%

861 861 812 812 -

x 10- 4 x 10- 6 x 10- 6 x 10- 5 • 10- 4 xl0 -4 x 10- 4 • 10- 4 • 10- 4 • 10- 4 • 10- 4 • 10- 5 x 10- 4 x 10- 4 x 10- 4 x 10- 4 x 10- 3 x 10- 4 x 10- 6 x 10- 5 • 10- 4 • 10- 5 x 10- 4 • 10- 5 x 10- 4 x 10- 4

CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL~90% CL=90% CL=90% CL=90% CL=90% CL=90%

932 926 927 915 852 838 773 756 768 751 654 631 866 852 717 698 863 929 924 848 769 764 648 862 712

CL=95%

38

MesonSummaryTable 1 CHARMED,STRANGEMESONS

I(J P) = 89

I D*(2007)~ I

/, J, P need confirmation.

(c=s=

Mass m = 2006.7 4- 0.5 MeV (S = 1.1) mD,o -- mDo = 142.12 4- 0.07 MeV Full width F < 2.1 MeV, C L = 9 0 %

D + = c~, D;- = ~s,

similarly for D;'s

D*(2007) 0 modes are charge conjugates of modes below. D*(2007) 0 DECAY MODES

Fraction ( r i / r )

D0/r 0 007

(61.9• (38.1•

I D~177

I(d P) = o ( o - )

p ( M eV/c)

% %

43 137

Massm=

c r = 148.6/~m

D + form factors r 2 = 1,60 4- 0.24 r v = 1.92 • 0.32 I - j E T = 0.72 4- 0.18 Branching fractions for modes with a resonance in the final state include all the decay modes of the resonance. Ds- modes are charge conjugates of the modes below.

D*(2010)- modes are charge conjugates of the modes below. Fraction ( r i / r )

D~~ +

(67.7• (30.7• ( 1.6•

D+~ ~ 0+7

p (MeV/c)

% %

39 38 136

Inclusive modes

(20

+{4 )% )% • +{8 7%

{(1+) I, _/, P need confirmation.

Mass m = 2422.2 4- 1 . 8 M e V Full width F = .1R . . .~+4.6 -3.5 MeV

non- K-Kanything

(04

•

e+anything

( 8

_+ 56 )%

r anything

(18

_+{5

+

(S=1.2)

D1(2420} 0 DECAY MODES

Fraction ( r / / r )

D*(2010) + ~r-

seen

355

D + ~r-

not seen

474

p (MeV/c)

K + K - fr +

r

D~(2460) 0 modes are charge conjugates of modes below. Fraction ( r i / r )

D + ~r-

seen seen

D*(2010) + ~r-

I

p (MeV/c) 503 387

I(JP) = 89

D;(2460)• I Massm= 2459i4MeV

( S = 1.7)

mD~(2460) • -- mD~(2460) o = 0.9 4- 3.3 M e V

(S = 1.1)

K+K*(892) 0

[xx]

3,3 • 0,9 ) %

[xx] [xx}

1.8 • 0.8 )%

f0(1710) ;r+ -~ K + K - T r + K + K - 7r+ nonresonant K ~ ~ 0 ~r+ K * (892) + ~ 0 K + K - ~ + 7r~

seen seen

508 390

S=1.3

7 • 4 )xlO -3 1.5 • 1.9 ) x 10 - 3 9 • 4 )• -3

[YY]

[xx]

( 4.3 •

1.4 )%

(9 • )% [~x] ( 6.7 • 2.3 )% [xx] < 2,6 % < <

[xx] <

K+ K - lr+ ~r+ Trp (MeV/c)

981 182

1.0 ) %

f0 (980) 7r+ K+'K~(1430) 0

9 2.8 ( 4.3 •

% % 1.5 ) %

(5.8 •

2.5)%

2.9 ( 8.3 •

% 3.3 ) x 10 - 3

[xx] (

~ + ~+ ~ D ~ ~+ O*0~ +

( 3.5 •

Hadronic modeswith a KK pair (including from a ~) 3.6 + 1.1 )% 4.4 4- 1.2 )% [qq] S=l.l [x~] 3.6 • 0.9 )%

K*(892)+K*(892) 0 K ~ K- ~r+ lr + non-K *+ ~ , o

D~(2460)- modes are charge conjugates of modes below. Fraction (Fi/F)

(2.o • o.5)%

[ww]

KO K-Tr+ ~+

Full width r = 2 5 + ~ MeV

D~(2460) + DECAY MODES

[~]

S=1.3

( 2.6 • 0,7 ) % ( 8,9 • 3.4 ) x 10- 3

~p+ ~ r + Ir0 3-body K + K - ;r+Tr0 non-r K+~%+Tr-

JP = 2 + assignment strongly favored (ALBRECHT 89B).

7%

( 4.6 • 1.9 ) x 10 - 3 ( 7 • 4 )%

r r/t+uz + T/(958)t+vt

K+K 0

( S = 1.2)

)%

Leptonic and semileptonic modes #+//# r+t~r

JP = 2 + assignment strongly favored (ALBRECHT 89B).

D~(241~) 0 DECAY MODES

(39

f/t+tJl ~I(958)~+/~ t

I(JP) = 89

M a s s m = 2458.9 4- 2.0 MeV Full width r = 23 4- 5 MeV

K~

K + anything

~1(2420)0 modes are charge conjugates of modes below.

I D;(2460)~ I

(13

K~

I(JP) =

Scale factor/ p Confidence level (MeV/c)

Fraction (r~/r)

D-+ DECAY MODES

K-anything

J D1(2420)0 J

(5=1.1) ( S = 1.1)

Mean life ~- = (0.496_0.009) +O.OLO x 10 -12 S

I, J, P need confirmation. M a s s m = 2010.0 4- 0.5 MeV ( S = 1.1) mD,(2010)+ - mo+ = 140.64 4- 0.10 MeV (S = 1.1) mD,(2OlO) + - mDo = 145.436 4- 0.016 MeV Full width r < 0.131 MeV, CL = 90%

D'(2010) :E DECAY MODES

1968.6 4- 0.6 MeV

mo~ - mD• = 99.2 4- 0 . 5 M e V

I(JP) = 89

I

II

CL=90% CL=90% CL=90%

CL=90%

1.18• 0.357%

( 3.0 + 3.0 ) x 10- 3 - 2,0

K + K - ~ r + ; r + ~ r - non-~

850 805 712 682 732 186 204 805 802 683 748 687 407 687 748 744 744 412 744 673 640 673

Hadronic modeswithout K's ~+=+=-

( 1.o + 0,4 )%

p0/r + f0(980)Tr + f2(1270)~ + fo(1500)Tr + -~ l r + T r - ~ + r + 7r+ ~r- nonresonant ~ + ?r+ ?r- ~r0 ,7~ +

w~ +

< [xx] [xx I [zz]

8

( 1.8 • 0.0 ( 2.3 + 1.3 ( 2.8 • 1.6 < 2.0 < 12 [xx] ( 1.7 • 0.5

• 10 - 4 )% ) x 10 - 3 )x10 -3 x 10 - 3 % )%

[xx] (2.8 • 1.1 )xlo -3

S=1.2 CL=90% S=1.7

CL--90% CL=90%

959 827 732 559 391 959 935 902 822

39

Meson SummaryTable /r +'a"+ 7i"+ / r - / r 71"+ 11-+ t r - / r 071"0 'r/p + r/Tr+~T03-body /r + / r + 1T+ 7--/r--/r 0 ~/'(958)7r + Ir + lr + ir + I t - l r - lr 0 7r0 r/(958)p + ~/'(958)Tr+Tr03-body

~)K + AC=

;'r+ e+ e-

E + p,+ It,-K + e+ eK -t 11,+ p.7r+ e• K+e•

{xx] {xx] [xx]

Modes with one < ( < [xx] ( < [xx] <

K 0/r + K+Tr+lr K+p 0 K*(892)07r + K +K + K-

K*(892)+#+#

[xx] [xx]

( 6.9 • 3.0 -(10.8 • 3.1 < 4 ( 4.9 • 3.2 ( 3.9 • 1.0 -(10.1 • 2.8 < 1.4

-

~

~r- e + e + /r--#+# + /r-- e +,u, + K- e+ e+ K-#+# +

K-e+# + K*(892)-#+/~ +

) x 10- 3 )% % )% )%

CL=90%

)% %

or three K's 8 x 1.o + 0.4 ) % 2.9 x 63 :E 2.8 ) • 6 x 5 x

CL=90% lo - 3

CL-90%

10 - 3 10 - 3 10 - 4 10 - 4

EL=90%

899 902 727 886 856 743 803 470 720

CL=90% CL=90%

916 900 747 773 628 607

1 weak neutral current (CI) modes, or Lepton number (L) violating modes [ss] < 2.7 x 10 - 4 CL=90% [ss] < 1.4 x 10- 4 EL=90% C1 < 1.6 x 10- 3 CL=90% C1 < 1.4 x 10 - 4 CL=90% Cl < 1.4 x I0 -3 CL=90% LF [ee] < 6.1 x 10- 4 CL-90% LF [ee] < 6.3 x 10 - 4 CL=90% L < 6.9 x 10 - 4 CL=90% L < 8.2 x 10 - 5 CL-90% L < 7.3 x 10 - 4 CL=90% L < 6.3 • 10 - 4 CL=90% L < 1.8 x 10 - 4 CL=90% L < 6.8 x 10- 4 CL=90% L < 1.4 x 10- 3 CL=90%

979 968 922 909 765 976 919 979 968 976 922 909 919 765

BOTTOM(B=+I)MESONS B + = ub, B ~ = db, ~ o = d b ,

B - = ~b,

similarly for B*'s

B-particle organization I Many measurements of B decays involve admixtures of B hadrons. Previously we arbitrarily included such admixtures in the B • section, but because of their importance we have created two new sections: " B • 0 Admixture" for 7"(45) results and "B+/B~176 A d m i x t u r e " for results at higher energies. Most inclusive decay branching fractions are found in the Admixture sections. B ~ ~ mixing data are found in the B ~ section, while Bs-B s ~--o mixing data and BB mixing data for a B~ ~ admixture are found in the Bs0 section. CP-violation data are found in the B ~ section, bbaryons are found near the end of the Baryon section. The organization of the B sections is now as follows, where bullets indicate particle sections and brackets indicate reviews. 9 B+ mass, mean life branching fractions 9 B0 mass, mean life branching fractions polarization in B ~ decay

r ~

l(JP)

B~

0(? ?)

=

JP is natural, width and decay modes consistent with 1 - .

9 B • B ~ Admixtures branching fractions

Mass m = 2112.4 4- 0.7 MeV ( S = 1 . 1 ) mD~:L - rno~ = 143.8 4- 0.4 MeV Full width r <

~ mixing

CP violation

9 B•176176

1.9MeV, CL=90%

Admixtures

mean life production fractions

D ; - modes are charge conjugates of the modes below.

branching fractions

D s9+ DECAY MODES

Fraction ( r i / r )

p (MeV/c)

D+'y D s+ 7r0

(94.24-2.5) %

139

(5.8•

48

%

9 B* mass

9 B~ mass, mean life

I Dn(2536)• I

/(JP) =

branching fractions

0(1+)

polarization in Bs0 decay

J, P need confirmation.

B~

Mass m = 2535.35 4- 0,34 4- 0.5 MeV Full width r < 2 . 3 M e V , C L = 9 0 %

0 mixing

B - B mixing (admixture of B 0' B 0)

D51(2536)- modes are charge conjugates of the modes below. mass, mean life

Ds1(2536)+ DECAY MODES

Fraction ( r i / r )

D* (2010) + K ~ D* (2007) 0 K + D+ K0 D0K + O~ + ~

seen seen not seen not seen possibly seen

I Da](2573)•I

p (MeV/c) 15o 169 382 392 389

branching fractions At end of Baryon Listings:

9 Ab mass, mean life branching fractions 9 b-baryon Admixture mean life

I(JP) = 0(??)

branching fractions

JP is natural, width and decay modes consistent with 2 + . Mass m = 2573.5 + 1.7 MeV Full width r = 15_+4s MeV Dgj(2573 ) - modes are charge conjugates of the modes below.

Djjr(2573) + DECAY MODES

Fraction ( r i / r )

D OK + D* (2007) 0 K +

seen not seen

p ( M eV/c) 436 245

II

40

Meson SummaryTable I(J P) =

89

I, J, P need confirmation. Quantum numbers shown are quark-model predictions.

B - modes are charge conjugates of the modes below. Modes which do not identify the charge state of the B are listed in the B4-/B 0 A D M I X T U R E section.

3.3

x 10- 4

CL=90%

2214

<

5

• 10- 4

CL=90%

2235

<

8

• 10- 4

CL=90%

2177

<

4

x 10 - 4

CL=90%

2198

<

5

x 10 - 4

CL=90%

2139

<

5

x 10 - 4

CL~90%

2195

D*s+ ~o

<

7

x 10 - 4

CL=90%

2136

D + al (1260) 0

<

2.2

x 10- 3

CL=90%

2079

Ds + a I (1260) 0

<

1,6

x 10- 3

CL=90%

2014

<

3.2

x 10- 4

CL=90%

2141

<

4

• 10- 4

CL-90%

2079

<

1.1

• 10- 3

CL=90%

2241

o~q,

D;+r O,+~o

The branching fractions listed below assume50% B0B 0 and 50% B + B production at the T(4S). We have attempted to bring older measurements up to date by rescaling their assumed T(4S) production ratio to 50:50 and their assumed D, Ds, D*, and ~ branching ratios to current values whenever this would affect our averages and best limits significantly.

o;+~o 0,+~*(892)o

Indentation is used to indicate a subchannel of a previous reaction. All resonant subchannels have been corrected for resonance branching fractions to the final state so the sum of the subchannel branching fractions can exceed that of the final state. p Scale factor/ Confidencelevel (MeV/c)

Fraction ( r i / r )

<

p+, ,~ s 0 D; + p ~

Mass rnB~ = 5279.0 4- 0.5 MeV Mean life r B • = (1,653 4- 0.028) x 10 -12 s Cr = 496 # m

B + DECAY MODES

D*s+ ~0

[pp] [pp] [pp]

t+utanything

-DOt+el. 9*(2007)~ Dl(2420)~ 9~(2460)0[+vt tr~

(lO.2 • )% ( 2.154-0.22)% ( 5.3 ::0.8 )% ( 6.6 4-1.6 ) x 10- 3 < 8 x 10 - 3

< [pp] < [pp] <

~ t + t,,~ pO~,+~ t e + I,'e

<

/z+z)#

<

T + t-'T

<

e+b'e7

<

/~+,u#7

<

-CL=90%

2.2 2.1 2.1 1,5 2.1

x x x x x

CL=90% CL=90% CL=90% CL=90% CL-90%

2638

5.7 2.0 5.2

x 10- 4

CL=90%

2340

x 10- 4

CL=90%

x 10- 5

CL=90%

-

2639 2638 -

D, D*, or Ds m o d e s ~ 0 ~r+

5.3:50.5 ) x 10- 3

9op+

1.34•

9 0K+ 901r+~+

7r-

~ o ~r+ ~r+ ~r- nonreson ant

9o~+po D 0 a1(1260) + D*(2010)-

lr+lr +

D-~r+Tr + D*(2007)%r + D * ( 2 0 1 0 ) + 7r~ D*(2007)~ + D * (2007) o 7r+ ~r+ 7rD * (2007)0 a1(1260) + D * ( 2 0 1 0 ) - 7r+ ~-+ 7r0

D*(2010)-~r+ ~r+ :r+ ~ D [ (2420) 0 ~-+ D;'(2420)0 p + 9 ~ ( 2 4 6 0 ) 0 ~r+ 9~(2460)0p + 9o D +

2.9:50.8 1.1:50.4 5 4-4 4.2 4-3.0 5 :54 2.1 4-0,6 < 1.4 ( 4.6 4-0,4 <

%

) x 10- 4 )% ) x 10- 3 ) x 10- 3 ) x 10- 3 ) x 10 - 3 X 10 - 3

CL=90% S=1.3

2289 2289 2209 2123 2247 2299 2256 2254 2183 2236 2062 2235 2217 2081

CL=90% CL=90%

1997 2064

CL=90%

1979

EL=90% CL=90%

(1.554-0.31) % ( 9.4 4-2,6 ) x 10- 3

( 1.9 4-0.5 )% ( 1.5 4-0.7 )% <

1

%

( 1.5 •

< < <

1.4

) x 1o- 3 x 10- 3

1.3

x 10- 3

4.7

x

10 - 3

( 1.3 4-0.4 ) %

1815

9 ~ D~ + 9*(2007)00 +

( 9

1734

( 1.2 4-0.5 ) %

1737

9 * ( 2 0 0 7 ) 0 O~ +

( 2.7 4-1.0 ) %

1650

9*(2007) 0 O*(2010) + D~ D*(2010) + + 9*(2007) 0 D + 9OD+ + o

0 s ~r

4-4

CL=90%

x 10- 4

CL=90%

2184 2171

<

4

• 10 - 4

CL=90%

2110

<

8

x 10 - 4

CL=90%

2222

D*s-~+ K+

<

1.2

x 10- 3

CL=90%

2164

D s lr + K * ( 8 9 2 ) +

<

6

x 10- 3

CL=90%

2137

D ; - ~r+ K * ( 8 9 2 ) +

<

8

x 10- 3

CL=90%

2075

J/~,(15) K + ~ + E J/~;(15) K * ( 8 9 2 ) + J/Vp(lS)Tr+ J/VJ(15)p+ J / ~ ( 1 5 ) a1(1260) + ~b(25) K*(892) + tb(2S) K + = + 7rXcl ( 1 P ) K +

Xcl(1P) K*(892)+

Charmonium m o d e s (10.0 -}-1.0 ) • ( 1,4 +o.6 ) x (1.484-0.27) x ( 5.1 4-13 ) x < 7.7 x < 1.2 x ( 5.8:51.0 ) x < 3.0 x ( 1,9 4-1.2 ) • ( 1.0 4-0.4 ) x <

K or K*

KOTr + K+~r o 7/' K + 7/K*(892) + 7/K + r/K*(892) +

) x 10- 3

< <

1.1 1.3

% %

CL=90% CL=90%

<

6.7

<

2.0

x 10- 3 x 10- 4

CL=90% CL=90%

2270

w K * (892) + K * (892) o ~r+ K * ( 8 9 2 ) + ;T0 K + ~r- ~r+ nonresonant K - ~ + ~r+ nonresonant K I ( 1 4 0 0 ) 0 ~r+ K~ (1430) 0 lr +

K+ pO KOp+

2.1

10- 4 10- 3 10- 3 lO - s 10- 4 10- 3

10- 3 10- 3 10- 3 x 10- 3

CL=90%

CL=90%

1.3

• 10 - 4

<

1.4

• 10 - 5

3.0

x 10- 5

CL=90% CL=90% CL=90% CL=90%

<

8.7

x 10- 5

<

4.1

x 10 - 5

<

9.9

• 10 - 5

<

2.8

x 10- 5

<

5.6

• 10 - 5

<

2.6

x 10 - 3

<

6.8

• 10 - 4

<

1,9

x 10 - 5

<

4.8

x

CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90%

K * ( 8 9 2 ) + ~r+ ~rK*(892)+p ~

<

i.I

• 10 - 3

<

9,0

x 10- 4

K1(1400)+p0

<

7.8

x

10- 4

K~(1430)+p 0 K+-~0

<

1.5

X

10 - 3

<

2.1

x 10 - 5

K+ K+ K+ K+

<

x 10- 5

< < <

7.5 8.79 1.29 2.0 5

• 10- 4 x 10- 4 x 10- 6

K + K - K + nonresonant K*(892) + K + KK*(892)+~b K1(1400) + K~(1430) +

<

3.8

x 10 - 5

<

1.6

x 10 - 3

<

4.1

< <

1.1 3.4

x I0 - 5 x 10- 3 x 10- 3

K + f0(980)

<

8

x 10 - 5

CL=90%

K+r

K * ( 8 9 2 ) + ~,

2614 2615 2528 2472 2587 2534

( 1.5 +0.7 --0.6 ) x 10- 5

CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=9O% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90%

K - ~r+ nonresonant K+Tr - nonresonant K*(892) 0 K- K +

1683 1612 1571 1727 1613 1414 1284 1115 909 1411 1265

modes

<

<

CL=90% CL=90%

10 - 4

( 2.3 4-1.1 ) x 10- 5 < 1.6 x 10 - 5 ( 6.5 4-1.7 ) x 10- 5

•K +

) x 10 - 3 x 10 - 4

1,7

2308 2238

x 10- 3

5

D~- 7r+ K +

,~(25) K +

10- 3 10- 4 10- 4 10- 5 10- 5

1.1

<

D:+K*(892) 0

J/~b(15) K + S e m i l e p t o n i c a n d leptonic m o d e s

<

<

10- 5

x 10 - 5

5.7:53.3 ) x 10- 5

2561 2562 2609 2451 2443 2559 2559 2556 2505 2389 2382 2592

2522 2516 2516 2466 2460 2339 2332 2524 2564

41

Meson SummaryTable 7.3

K1(1270)+7

<

K1(1400)+7

< 2.2 1.4

x 10 -3 x 10 -3 x 10 -3

CL=90% CL=90% CL=90%

2486 2453 2447

K~(1430) + 7

<

K*(1680)+7 K~(1780)+7

< <

1.9 5.5

x 10 -3 x 10 -3

EL=90% CL=90%

2361 2343

K~(2045)+7

<

9.9

x 10 - 3

CL=90%

2243

F~

l(JP) 89

I, J, Pneedconfirmation. Quantum numbersshown are quark-model predictions. Mass

<

2.0

x 10- 5

CL=90%

2636

/r + 1[+ ~ ' pO 7r+

< <

1.3 43

x 10- 4 x 10 - 5

CL=90% CL=90%

2630 2582

< < < <

1,4 2.4 4.1 8.9

x 10 -4 x 10 - 4 x 10-5 x 10 - 4

CL=90% EL=90%

2547 2483

<

7.7

~+ fo(980) 1[+ f 2 ( 1 2 7 0 )

1[+ 7r- Ir + nonresonant 1[+ ~r0/r 0

p+~r0 7[+/r-- 7r+';T0

<

p+pO al(1260)+~r 0 a1(1260)01r + {.,.,'/r+ u2p + T/7r+ T/l[ +

flip+

rlp+ <~Ir+ Cp+

lf+lr+'lr+~"

~T

pOa1(1260)+ p0a2(1320)+ 1[+ ~r+ / r + ~ - ~'-- lT0 a1(1260)+ a1(1260) 0

CL=90%

2631

x 10 - 5

CL=90%

2582

10 - 3 10 - 3

EL=90% EL=90%

2621 2525

10 -3

CL=90% CL=90% CL-90% EL=90% CL=90% CL=90% CL=90% CL=90% CL=90%

CL=90% CL=90%

2494 2494 2580 2609 2550 2493 2554 2608 2434 2411 2592

CL=90%

2335

4.0 < 1.0 < 1,7 < 9.0 < 2.3 < 6.1 < 1.5 < 3.1 < 4.7 < 3.2 < 5 < 1.6 < 8.6 < 6.2 < 7.2 < 6.3

x x x x x

<

%

1.3

-

CL=90%

10- 4 10- 5

x 10 - 5

x 10 - 5 x 10 - 5 x 10 - 5 x 10- 5 x 10 - 6 x 10 - 5 xl0 -4 x 10 - 4 x 10 - 4 x 10 - 3

CL=90% CL=90%

BO-~ ~ mixing parameters

Xd = 0.174 + 0.009 AmBo = mBoH -- mBoL = (0.472 + 0 . 0 1 7 ) x 1012 T~ S- 1 Xd = AmBO/['BO = 0 . 7 3 0 • 0 , 0 2 9

CP violation parameters

Re(CBO)/(l+l~Bol 2)

=

0.002 • 0.007

sin(2~) = 0.9 • 0.4 ~ 0 modes are charge conjugates of the modes below. Reactions indicate the weak decay vertex and do not include mixing. Modes which do not identify the charge state of the B are fsted in the B • 0 ADMIXTURE section. The branching fractions listed below assume 50% B 0 B 0 and 50% B + B production at the T(45). We have attempted to bring older measurements up to date by rescaling their assumed T(4S) production ratio to 50:50 and their assumed D, Ds, D*, and ~b branching ratios to current values whenever this would affect our averages and best limits significantly. Indentation is used to indicate a subchannel of a previous reaction. All resonant subchannels have been corrected for resonance branching fractions to the final state so the sum of the subchannel branching fractions can exceed that of the final state.

Charged particle (h 'l:) modes h • = K • or ~r•

5279.4 + 0.5 MeV

(S = 1.1) Mean life ~'B0 = (1.548 • 0.032) x 10 -12 s or = 464 #m 'TB+/-rBO = 1.060 • 0.029 (average of direct and inferred) "rB+/'rso = 1.062 + 0.029 (direct measurements) (inferred from branching fractions) TB+/'rBO ---- n . . .Q~+0.15 . --0.12

Ught unflavored meson modes 1[+/r 0

mBo=

mBo -- mB• = 0.33 • 0.28 MeV

B 0 DECAY MODES

h+/r 0

( 1.6 +0.7 ) x l O - 5 -0.6 2.50 x 10- 5

~Jh+

< <

1.6 5.3

x 10- 4 x 10- 5

CL=90% CL=90%

2439 -

p-p~T+ 1[+ n--p~K+nonresonant

<

<

5.2 8.9

10- 4 10- 5

EL=90% CL=90%

2369 -

pA

< <

2.6 2,0

x x x x

<

3.8

<

1.5 ( 6.2 •

10- 6 10 - 4 x I0 - 4 x 10 -4

CL=90% CL=90% CL=90% EL=90%

2430 2367 2402 2402

p ~ r + nonresonant

p-A'K+'K ~0 p .4++~ Acp~T+

) x l 0 -4

A c pTr+'r

<

3.12

x 10 - 3

CL=90%

AcPTr+~+Ir-

<

1.46

x 10 - 3

EL=90%

A c P1[+1[+'ir-lr 0

<

1.34

%

CL=90%

81 B1 81 B1

K*(892) + e+ e-

81

K*(892)+#+# lr + e + # -

< < < < < <

[PP] (10.8 • [PPl ( 2.10•

D*(2010)- ~+ ut

[PP} ( 4 . 6 0 •

p-~,+lJ t

[pp]

3.9 9.1

x 10 - 3 x 10 - 3

CL=90% CL=90%

6 5.2 6.9 1.2 6.4 6.4

x 10 - 5 xl0 -6 x 10 - 4 x 10 - 3 x 10 - 3 x 10 - 3

EL=90% EL=90% EL=90% CL=90% CL=90% CL=90%

x 10 - 3

CL=90%

( 1.8 •

K + anything

(78

2612 2564 2560 2637 2637

%

) x 10 - 4

•

)%

D, D*, or D s modes D-'K + O-p +

( 3.0 • ( 7,9 • < 1.6

)xl0 -3 ) x 10 - 3 x 10 - 3

2.76• 8.0 •

x 10 - 3 xl0 -3

nonresonant

3.9 • 1.1 •

x 10 - 3 x 10 - 3

2287 2207

D-a1(1260) + D*(2010)-1[+~ ~ D*(2010)-p + D*(2010)-~+~+~ ( D * ( 2 0 1 0 ) - T r + ~ + 1 [ - ) non-

6.0 • 1.5 •

x 10 - 3 %

2121 2247

6.8 •

x 10-3

7.6 •

x 10 - 3

0.0 •

x 10 - 3

2235

( 5.7 •

) x 10 -3

2151

D-1[+'tr+'lr -

2633 2616

)%

Inclusive modes

D * ( 2 0 1 0 ) - ~r+

2638

p (MeV/c)

( 2.6 _+016 } x l O - 4

~r-t+ut

9 0/r + 1 [ -

Lepton Family number (LF) or Lepton number (L) violating modes, or ZIB -- 1 weak neutral current (81) modes ~+ e + e ~+#+,u,K + e+ e K+IJ,+p, -

D-l+ut

t+utanything

Baryon modes p~r +

Scale factor/ Confidence level

Fraction ( r i / r )

(D-~+~r+~ D-/r+,o 0

-)

resonant D*(2010)-1[+p 0

CL=90%

2306 2236 2301 2254 2287

2181 S=1.4

2235

K + e- I~+

B1 LF LF LF LF

<

6.4

x 10- 3

CL=90%

2615 2615

D~(2460)-p +

<

4.9

• 10 - 3

CL=90%

1['- e + e + ~'-- /,r /J+

L L

< <

3.9 9.1

x 10 - 3 x 10 - 3

CL=90% EL=90%

2638 2633

D- D +

<

1.2

x 10 - 3

EL=90%

D-D +

( 8.0 •

) x l O -3

1812

I r - e+ p,+

LF

<

6.4

) x 10-3

1735

<

3.9

D-D's+

( 1.0 •

)%

1731

K-#+# + K-e+# +

L

<

EL=90% EL-90%

)%

<

xl0 -3 xlO -3

( 2.0 •

LF

9.1 6.4

2637 2616 2612 2615

( 9.6 •

L

CL=90% EL=90%

0*(2010)-D +

K - e+ e+

xlO -3 x 10 - 3

~+ e - # + K+e+p, -

< < < 6.4

D*(2010)- a1(1260) + D*(2010)-1[+1[+1[-Ir ~

(1.30•

D~(2460)-7r +

( 3.5 • < 2.2

D*(2010)-D;

+

%

2061

)% x 10 - 3

EL=90%

2218 2064 1979

1649

D s+ 1 [ -

<

2.8

x 10- 4

EL=90%

2270

D=s+'/rO+sp -

<

5

x 10- 4

CL=90%

2214

<

7

x 10 - 4

EL=90%

2198

D; + p-

<

8

x 10- 4

CL=90%

2139

42

Meson SummaryTable D + al ( 1 2 6 0 ) -

<

2.6

x 10 - 3

CL=90%

2079

K1(1270)~

<

7.0

x 10 - 3

CL--90%

2486

D; + a1(1260)D; K +

<

2.2

x 10- 3

CL=90%

2014

K1(1400)~

<

2.4

x 10 - 4

CL=90%

2242

K~(1430)0'7

< <

4.3 4,0

X 10 - 3 • 10- 4

CL=90% CL=90%

2453 2445

K*(1680)07 K~(1780)07

<

2.0

• 10 - 3

CL=90%

2361

<

1,0

%

CL=90%

2343

K,~ (2045)0 7

<

4.3

x 10 - 3

CL=90%

2244

D*s - K +

<

1.7

x 10- 4

CL=90%

2185

D~- K * ( 8 9 2 ) +

<

9.9

x 10- 4

EL=90%

2172

D~- K*(892) +

<

1,1

x 10- 3

EL=90%

2112

D~" ~r+ K ~

<

5

x 10- 3

EL=90%

2221

D ~ - ~r+ K ~

<

3.1

• 10 - 3

EL=90%

2164

/ r + ,/r -

D~- ~r+ K * ( 8 9 2 ) ~

<

4

x 10 - 3

CL=90%

2136

D*~- ~r+ K * ( 8 9 2 ) ~

<

2.0

x 10 - 3

CL=90%

2074

~T07r0 r//r o

~ ~ro

<

1,2

x

10- 4

CL=90%

2308

< <

3,9

1.3

x 10- 4 x 10 - 4

CL=90% CL=90%

2238 2274

<

9,4

X 10 - 4

CL=90%

2198

< <

5.1 4.4

• 10 - 4 x 10 - 4

CL=90% CL=90%

2235 2256

D*(2007)~ ~ D * ( 2 0 0 7 ) ~ T/ D * ( 2 0 0 7 ) 0 ~'

< <

5.6 2.6

<

1.4

x 10- 4 x 10- 4 X 10 -3

CL=90% CL=90% CL=90%

2183 2220 2141

D* (2007)~

<

7.4

X i0 -4

CL=90%

2180

~ o p0 ~ 0 ~/ DOoj ~ * ( 2 0 0 7 ) 0 ;TO

( 6.2 +4.1 - 3 . 1 ) x 10 - 4

O*(2010) + D*(2010)-

LIl~t unflavored meson modes

7/t 7r0

~/lpO

oJfi ojfiI ~pO b2~9

~o

1711

O*(2010) + D-

<

1.8

x 10 -3

CL=90%

0(*)o~(*)o

<

2.7

%

CL=90%

1790 -

@po

Charmonium modes J/%b(1S)K~ J/~(IS) K + ~rJ/~(I5) K * ( 8 9 2 )

0

( 8.9 - - 1 . 2 ) x 10 - 4

1683

( 1,2 --0,6 ) x 10 - 3 (1,50• x 10 - 3

1652 ]570

It+ ~ - ~r0

polo p=~~r--

J/~(lS)~ ~ J/@(]s)v

<

5,8

x 10 - 5

CL=90%

1728

<

1.2

x 10 ~3

CL=90%

1672

~r+/r- if+/r pO po

J/~b(IS)p0

< < < <

2.5 2.7 8 1

x x x x

CL=90% CL=90% CL=90% CL=90%

1614 1609 1283 1238

a1(1260)q: ~r+ a 2 ( 1 3 2 0 ) q: ~ + /r+ / r - /to /r 0

J/~(lS)~ r

K~

~b(25) K + ~r~(2S) K* (892) 0 Xc1(1P) K ~

•

(1 P) K* ( 8 9 2 ) 0

10 -4 10- 4 10- 4 10 - 3

( 9.3 --2.3 )x 10- 4 < <

2.7 2.1

x 10- 3 x 10- 3

1113 CL-90% CL=90%

1411 1263

K or K* modes ( 1 3 +0.5 - 0 . 4 ) x 10 - 5

K+~r K o ~ro

<

4,1

(

~/K 0

x 10 - 5

2615 EL=90%

4.7 --2,2 + 2 . 8 ) x 10 . 5

2614 2528

q'K*(892) ~ ~/K*(892) ~ ~,K o wK o

< < < <

3.9 3.0 3.3 5.7

x x • x

10 - 5 10 - 5 10- 5 10 - 5

EL=90% CL=90% CL=90% CL=90%

2472 2534 2593 -

w K* (892) 0

< < < < < <

2.3 4.3 1.7 3.5 3.9 3.6

x x x x x x

10 - 5 10 - 6 10 . 5 10- 5 10- 5 10- 4

CL=90% CL=90% CL=90% CL=90% CL=90% CL=90%

2593 2592 2559 2559 2523

<

7.2

x 10- 5

CL=90%

2562

<

2.8

x 10 - 5

CL=90%

2562

<

2.6

x 10 - 3

CL-90%

2445

< < [aaa] < < <

1.3 3.1 2.3 1.4 4.6

x x x x x

10 - 3 10 - 5 10- 4 10- 3 10- 4

CL=90% CL=90% CL=90% CL=90% CL=90%

2522 2516 2600 2556 2504

< < <

1.7 1.1 2.3 6.1

x • x x

10- 4 10 - 3 10 - 4 10 - 4

CL:90% CL=90% CL=90% CL=90%

2467 2451 2471 2466

<

2.1

x 10 - 5

CL:90%

2459

<

3.0

x 10 - 3

CL=90%

2389

K~(14~0)~ ~

< <

5.0 1.1

x 10- 3 x 10 - 3

CL=90% CL=90%

2339 2380

K~(1430) 0

<

1.4

x 10 -3

CL=90%

2330

K+K K o ~o K+p K o pO K ~ fo ( 9 8 0 ) K * ( 8 9 2 ) + ~rK*(892)~ 0 K ~ ( 1 4 3 0 ) + ~r-

KOK+ K -

K~$ K - ~ r + ;,r+ ~rK*(892)~ ~rK*(892)~ 0 K * ( 8 9 2 ) ~ fo(980) /(1 ( 1 4 0 0 ) + ~ K - a I (1260) + K*(892) 0 K + KK*(892) ~ Kl(1400)~

~

K1(1400)%

K*(892)07

[aaa] <

( 4.0 +1.9 )x 10 -5

2564

p+ pa1(1260)~ 0 ~r 0 ~ + / r + ~r- ~1-- 7r0 al(1260)+p al (1260)0 pO

7r+ 7r+ ~r+ ~--- ~ - ; r a1(1260) + a 1 ( 1 2 6 0 ) 7r+ ~ + / r + ~r- ~r- ~ - ~r0

< <

1.5 9.3

x 10- 5 x 10 - 6

CL=90% CL=90%

2636 2636

< < <

8 1.8 1.1

<

4,7

• 10 - 6 • 10 . 5 x 10 - 5 • 10 - 5

CL=90% CL=90% CL=90% CL=90%

2609 2582 2551 2460

< <

2.7 2.3

x 10 - 5 • 10 - 5

CL=90% CL-90%

2522 2493

< < <

1.3 1.2 6.0

x 10 - 5 • 10 - 5 x 10 - 5

CL=90% CL=90% CL=90%

2554 -

< < < <

1.1 1.9 5 9

x • • •

CL=90% CL--90% EL=90% EL=90%

--

<

3.1

x 10 - 5

CL:90%

--

< <

13 2.1

• 10 - 5 • 10 - 5

EL=90% CL=90%

-

< <

1.2 7,2

• 10 - 5 • 10 - 4

CL-90% CL=90%

2435 2631

10 - 5 10 - 5 10 - 6 10 - 6

<

2.4

x 10 - 5

CL=90%

2582

[eel <

8.8

• 10 - 5

EL=90%

2582

< < [eel <

2.3 2.8 4.9

• 10 - 4 • 10 - 4 x 10 - 4

EL=90% EL=90% CL=90%

2621 2525 2494

lee] < < < < <

3.0 3.1 2.2 1.1 1.4

x • • x x

10 - 4 10 - 3 10 - 3 10 - 3 10 - 5

CL=90% CL=90% CL=90% CL-90% CL-90%

2473 2622 2525 2494 2580

< <

9.0 3.4

x 10- 3 x 10- 3

CL=90% CL-90%

2609 2434

< <

2.4 3.0

x 10 - 3 x 10 - 3

CL=90% CL=90%

2434 2592

<

2.8

x 10 - 3

CL=90%

2336

<

1.1

%

CL=90%

2572

Baryon modes p~ p~r+~ p~';,r-

~A .aozo A++~--

~ - - z~++

< <

7,0 2.5

x 10 - 6 x 10 - 4

CL--90% CL=90%

2467 2406

< < <

1.3 3.9 1.5

x 10 - 5 x 10- 6 x 10 - 3

CL=90% EL=90% CL=90%

2401 2334

< <

1,1

• I0 - 4 • 10 - 3

EL=90% CL=90%

2334 1839 2021

1.0

( 1.3 =E0.6 ) x 10 - 3

Ac p~r+Tr-

~-p

<

2.1

x 10 - 4

EL=90%

A~- pTr 0

<

5.9

x 10 - 4

CL=9O%

-

~ - p~r+ ~r- ~ro ~ - pTr+ ~ - 7r+ 7r-

<

5.07

x 10 - 3

CL=90%

-

<

2.74

x 10 - 3

CL=90%

--

Lepton Family number (LF) violating modes, or &B = I weak neutral current (BI) modes 77 e+e #+#-

81

< <

3.9 5,9

x 10 - 5 • 10 - 6

CL=90% CL=90%

2640 2640

x 10 -7 x 10 - 4

CL=90% CL=90%

2637 2616 2612 2564 2559 2244

B1

<

6.8

K ~ e+ eKO#+# -

81

<

3.0

81

<

3.6

x 10 - 4

K*(892) 0 e+ eK * ( 8 9 2 ) 0 ,u.+ # -

81

<

2.9

• 10 - 4

BI

< 4.0

K*(892) ~ u~ e--/z T e--,1-T

B1

<

1.0

x 10 - 6 x 10 - 3

CL=90% CL=90% CL=90% EL=90%

LF LF LF

{eel <

3.5

x 10 - 6

CL--90%

2639

[eel < [ee] <

5.3 8.3

x 10 - 4 • 10 - 4

CL=90% CL=90%

2341 2339

p - - ..rzF

43 Meson S u m m a r y Table

I B•

Charmonium modes B -~ J/~b(15)anything 1.15• % B ~ J/~(1S)(direct) any8.0 4-0.8 ) x 10- 3

ADMIXTURE I The branching fraction measurementsare for an admixture of B mesonsat the T(45). The values quoted assume that B(T(4S) -~ BB) = 100%.

thing B -~ ~b(2S)anything

For inclusive branching fractions, e.g.. B ~ D4- anything, the treatment of multiple D's in the final state must be defined. One possiblity would be to count the number of events with one-oPmore D's and divide by the total number of B's. Another possibility would be to count the total number of D's and divide by the total number of B'S, which is the definition of average multiplicity. The two definitions are identical when only one of the specified particles is allowed in the final state. Even though the "one-or-more" definition seemssensible, for p~actical reasons inclusive branching fractions are almost always measured using the multiplicity definition. For heavy final state particles, authors call their results inclusive branching fractions while for light particles some authors call their results multiplicities. In the B sections, we list all results as inclusive branching fractions, adopting a multiplicity definition. This means that inclusive branching fractions can exceed 100% and that inclusive partial widths can exceed total widths, just as inclusive cross sections can exceed total cross sections.

B -~ Xcl(1P)anything B --* Xcl(1P)(direct) anything

B -~ Xc2(1P)anything

Semileptonlc and leptonlc modes [bbb] (10.414-0.29) %

B -~ e+z, eanything B -~ ~ e + z , eanything

<

B -~ #+upanything B -~ t+etanything B -* D - t + u t a n y t h i n g

[bbb] [pp,bbb] [pp] [pp] [pp,ccc]

B --* D ~

B ~

1.6 x 10- 3 10.3 4-0.5 )%

-D**~.+u l

B ~

D~t+utanything +

D* ~r~+ v l anything B -~ D ~ ( 2 4 6 0 ) t + ~ , t a n y thing B ~ D*-Tr+l+ulany thing B -~ D ~ - ~ + u t a n y t h i n g

B --~ D~g+L, t K + a n y -

6.5 (

x 10- 3

D4-anything D~176 D*(2010)• D*(2007)~ D~anything

B -~

D(*)D(*) K ~ +

D(*)~(*)K

CL=95%

c~s

B -~ B -*

Ds(*)D(*) D* D*(2010)4-

B-~

DD*(2010)4-+

x lO - 3

CL=90%

B-~

A~- e + a n y t h i n g

6

x lO - 3

CL=90%

B-~

AcPanything

B-~

"AcPe+Ve

[pp] < [pp] ( [pp] ( [pp] (

9

x lO - 3

CL=9O%

B-~

~-

(

)% )% )% )% )%

B--'

D~(*)•177

B ~

D"(2010)'),

( 22 4-4 ( 4.9 • [ee] < 5.9 [ee]< 5.5 [ee] < 3.1

B -* D +Tr-, D's+ 7r-,

o,+p- o;+p o,+30 o;+3o, o+~, o;§

( 9

[ee,ddd]

)% )% x 10- 3 xl0 -3 x 10- 3

CL=90% eL=90%

)% )% )%

•

)% )%

•

)%

4.1 8.3 1.2 3.0 1.0 2.3 • 6.8 4.4

x 10- 4 x 10- 4 x 10- 3 x 10- 3 x 10- 3 ) x 10- 4 % x 10- 4

CL=90% CL=90% CL=90% CL=90% CL=90% CL--90% CL=90%

6.2 +2.1 ) x 10- 4 -2.6

EL-90% S=1.8 EL=90%

-

B__,

_

B--, B--,

CL=90% CL=90% CL=90%

1.1 5

x 10- 3 x 10- 4

CL=90% CL=90%

<

9.5

x 10- 3

CL=90%

CL=90%

1.5 4.2:1:2.4

x 10- 3 x 10-3

CL=90%

(

9,6

x 10- 3

CL=90%

x 10- 3 xl0 -3

EL=90%

( 4.6 4-2.4 < (

B(-O-~ --~+)

x 10- 3

3.6 4-0.7 ) %

1.5 1.4 4-0.5

4.5 +1.3 -1.2

x 10- 4

x 10-4

B(_--c+ --, - - - , . , r + , + ) p/~anything p / ~ ( d i r e c t ) anything A/Aanything ---/~+ anything baryons anything p~anything

[eel [ee] [ee] [ee]

A~ /-Apanything

[eel

8.0 4-0.4 )% S.5 4-0.5 ) % 4.0 4-0.5 ) % 2.7 4-0.6 ) x 10- 3 6.8 • ) % 2.474-0.23) % 2.5 • )% 5 x 10- 3

-

B--*

-

e--+

-

B___,

-

Lepton Family number (LF) violating modes or AB = 1 weak neutral current (BJ) modes B1 < 5.7 x 10- 5 CL=90% B --~ e + e - s B1 < 5.0 x 10- 5 CL=90% B ---* # + # - s B -~ e4-#~s LF < 2.2 x 10- 5 CL=90%

+_5 )%

< [ee] <

3.2

<

--+anything •

6.4 4-1.1 ) %

(

<

anything

--~.anything

x

D ; + p O , D s+ W,

Ds1(2536) + a n y t h i n g

( <

~__~N(N=porn)

S=1.1

D;+ ~ B ~

• • • 4-4

Light unflavored meson modes [ee,eee] (358 4-7 )% ( 176 4-1.6 )% ( 21 4-5 )% < 81 % ( 35 4-0.7 )% < 2.2 x 10. 5

~_anything

B B B

7.1 +2:7 ) %

[ee,ddd]

e ---* D O •

D +p0

[ee,ddd]

4-1.9 :t:2.9 4-1.6 4-2.7 4-2.5

(

~-anything

6.0 4-0.5 )% lO :1:4 ) x 1 0 - 3 4.4 4 - 0 . 5 ) %

24.1 63.5 22.7 26.0 10.0

< <

e --~ A ~ a n y t h i n g

9

[ee]

D'D4-

- * lr4- anything --* ~/anything -~ po anything -~ ~ anything --* ~b anything B - ~ q~K*(892)

[pp] < [pp] <

( ( ( ( (

x 10- 3 x 10- 3

Baryon modes

1.oo4-o.34)%

•

b~

K~(2045)~,

< < < < <

B-~ K;(1780)~

B B B B B

D, D', or D s modes B--, B ~ B -+ B -~ B-~

e-~

- [ee]

B --+ T/~anything

thing

B ~ D~+vtK~ B - ~ K+ e+ ulanything B -~ K - l + u l a n y t h i n g B - ~ K~176

K2(1770)-7

78.9 66 13 64 18 14.6

[ee]

B-~ b-* ~gluon B -~ T/anything

2.3 4-0.4 ) % <

B--,

[ee]

(

S=1.2 CL=90%

10.454-0.21) % 2.7 4-0.8 ) % 7.0 • )% 2.7 4-0.7 ) % 7.4 4-1.6 ) x 10- 3

B ~ D1(2420)t+vtany thing

3.8 9

K or K* modes B --* K4-anything B -~ K + a n y t h i n g B --+ K - a n y t h i n g B -~ K ~ 1 7 6 B -~ K * ( 8 9 2 ) • B--+ K * ( 8 9 2 ) ~ 1 7 6 thing B - ~ K1(1400)~ e - - + K~(1430)3,

Scale factor/ P Confidencelevel (MeV/c)

Fraction ( r i / r )

< <

B --* % ( I S ) a n y t h i n g

modes are charge conjugates of the modes below. Reactions indicate the weak decay vertex and do not include mixing.

B DECAY MODES

3.5 4-0.5 ) x IO- 3 4.2 4-0.7 ) x 10- 3 3.7 • ) x 10- 3

-

AAanything

<

CL=90%

44

Meson SummaryTable

I B•176176

ADMIXTURE

I

These measurements are for an admixture of bottom particles at high energy (LEP, Tevatron, SpaS). Mean life r = (1.564 4. 0.014) x 10-12 s Mean life T = (1.72 4, 0.10) x 10-12 s Charged b-hadron admixture Mean life T -- (1.58 4, 0.14) x 10-12 s Neutral b-hadron admixture

I~Tbl/%,~

The branching fraction measurements are for an admixture of B mesons and baryons at energies above the T(4S). Only the highest energy results (LEP, Tevatron, SpaS) are used in the branching fraction averages. In the following, we assume that the production fractions are the same at the LEP and at the Tevatron.

~

-~o D Oanything

[ee]

(

D O D • anything

[eel ( 27_+~:o 8)% x 10 - 3 CL=90% [eel < 9

b-baryon BC

38.9 38.9 10.7 11.6

• • • • --

1.3 1.3 1.4 2.0

[ee]

(

3.0 + 1.1 _ 0.9)%

D* (2010) + D T anything

[ee]

(

2.5 + 1.2 1.o) %

D*(2010)• D~(2460)~

[~]

( 1.2 • 0.4 )% ( 4.7 ~ 2.7 )%

Semileptonic and leptonic ( 23.1 • LOp] ( 10.73:1: ( 10.86•

modes 1.5 )% 0.18)% 0.35) % 0.29, o/ 0.25/ /o 0.29)% 0.6 ) % 0.29) %

-~j t+ utanything

( 10.95 + LOp] ( 2.02• LOp] ( 6.6 • Lop] ( 2.76:t: [pp, fff] seen

O~ t + utanything

[pp, fff]

l+=,lanything e+ueanything # + =,~anything

D-t+=,tanything D~ O*-s

D~(2460) 0 ~+ v t anything D ~ ( 2 4 6 0 ) - s =,l anything char,less t-Pt T+=,Tanything ~--* l-~tanything

Pion modes (397 ~: 21 [eee] (278 ~:60

Baryon modes ( 13.1 ~: 1.1 ) %

charged anything

Other modes [eee] (497 4,-7 (

hadron + h a d r o n -

(

char,less

A/Aanything b-baryon anything

seen

seen seen LOp] ( 1.7 • 0.6 ) x 10- 3 ( 2.6 • 0.4 ) % LOp] ( 0.3 • 0.4 ) %

-

-

)% )%

p/~anything

_

s=1.1

modes ( 1.16• 0.10) % ( 4.8 ~: 2.4 ) x 10- 3 ( 1.8 ~: 0.5 )%

K or K * modes ( 3.1 d: 1.1 ) x 10- 4 (74 • 6 )% ( 29.0 9 2.9 )%

~ + anything ~o anything

)%

1.7 + 1.o ) x 1o- s - 0.7 7 :t:21 ) x l O - 3

Baryon modes ( s.9 :L o . 6 ) % ( 10.2 ~ 2.8 ) %

A B = 1 weak neutral current (131) modes B1 < 3.2 • 10 - 4 CL=90%

I(J P) = } ( 1 - ) I, J, P need confirmation. Quantum numbers shown are quark-model predictions. Mass m B, = 5325.0 4. 0.6 MeV roB, -- m B = 45.78 4- 0.35 MeV

DECAY M O D E S

=,anything

( 18 :1: s )% ( 9.7 • 2.9 )% [eee] (117 ~: 4 )%

b-baryon) = 100 %.

)% )% )% )%

( 23.7 9 2.3 ) % ( 17.3 ~: 2.0 ) % ( 5.0 :E 1.5 ) %

D O D*(2010) • anything

#+#-anything ( ( ( (

%

[ee] ( 3.3 +_ 1.6 L3)%

K • anything K 0 anything

The notation for production fractions varies in the literature (fd, dBO, f(b ~ ~0), Br(b ~ ~0)). We use our own branching fraction notation here, B(~ ~ B0).

B+ B~ Bs~

5.1 + 2.0 _1.8)

D*(2010) :F D ~ anything

Xcl(1P)anything

Scale factor/ P Confidence level (MeV/c)

B 0) -F B(b ~

( 4.0 _+ 2:3 ) %

C h a r , on•

The production fractions for weakly decaying b-hadrons at high energy have been calculated from the best values of mean lives, mixing parameters, and branching fractions in this edition by the LEP B Oscillation Working Group as described in the note "Production and Decay of bFlavored Hadrons" in the B ~c Particle Listings. Values assume B 0) B 0) §

[ee]

J/~(1S)anything ~(2S)anything

P R O D U C T I O N FRACTIONS

e +) = e ( b - B +) -t- B(b ~

D :F D ~ anything

~sanything Acanything ~/canything

The modes below are listed for a b initial state, bmodes are their charge conjugates. Reactions indicate the weak decay vertex and do not include mixing.

B(b~ B(b ~

[eel ( 9.1+_~:~)%

_

For inclusive branching fractions, e.g., B ~ D • anything, the treatment of multiple D's in the final state must be defined. One possiblity would be to count the number of events with one-or-more D's and divide by the total number of B's. Another possibility would be to count the total number of D's and divide by the total number of B's, which is the definition of average multiplicity. The two definitions are identical when only one of the specified particles is allowed in the final state. Even though the "one-or-more" definition seems sensible, for practical reasons inclusive branching fractions are almost always measured using the multiplicity definition. For heavy final state particles, authors call their results inclusive branching fractions while for light particles some authors call their results multiplicities. In the B sections, we list all results as inclusive branching fractions, adopting a multiplicity definition. This means that inclusive branching fractions can exceed 100% and that inclusive partial widths can exceed total widths, just as inclusive cross sections can exceed total cross sections.

Fraction (Fi/F)

D O Ds• anything

D • D:F anything D - anything D*(2010) + anything D 1(2420) 0 anything

"/'charged b-hadron/Tneutral b-hadron = 1.09 4, 0.13 = -0001 4, 0.014

DECAY MODES

Charmed meson and baryon modes ( 60.5 ~: 3.2 )%

D~

B ~ DECAY MODES

Fraction ( r i / r )

B "~

dominant

p (MeV/c) 46

45

Meson Summary Table

II

IIrEi

BOTTOM, STRANGE MESONS

(B= -I-1,S= :F1) e s~ = sb, ~

= ~b,

similarly for B;'S

I(J P)

= 0(0-)

BOTTOM,

il

CHARMED MEsoNs

(B-- C=-I-1)

B + -- cb, B c = "~b,

similarly for Bc'S

I(J P)

= 0(0-) I, J, P need confirmation. Quantum numbers shown are quark-model predicitions.

I, J, P need confirmation. Quantum numbers shown are quark-model predictions. Mass m o -- 5369.6• 2.4 MeV Bs Mean life r -- (1.493 • 0.062) x 10 -12 s

Mass m = 6.4 • 0.4 GeV Mean life

= (0.461~:~) • 10-12 5

B~- modes are charge conjugates of the modes below.

CT = 448 Fm B~

mixing parameters

XB

at high energy -o =mo -mo

Am

Bs

BsH

Xs AmeolrBo =

B + DECAY MODES

fdXd+fsXs BsL

>

-- 0.118 • 0.005 10.6x1012T~s -1,CL=95%

> 15.7, CL = 95~

Xs > 0.4980,CL = 95%

duction fraction.

(10.7 4- 1.4)% and the rest assume B(b ~

B 0) =

B 0) = 12%.

The branching fraction B(Bs0 ~ D~l+vlanything) is not a pure measurement since the measured product branching fraction B(b ~ BsO) x B(Bs0 ~ D~t+vlanything ) was used to determine B(b ~ Bs0), as described in the note on "Production and Decay of b-Flavored Hadrons." P

B~SDECAY MODES

Fraction ( r i / r )

D~- anything

(92

D ; t+ ulanything

[~g]

D;" 7r+

< 13

Ds (*) + Ds (*)J/~(15)r J/'r 0 J/'C(1S)rl

<

~'+ ~ ~'0/r0 ~T 0 //T/ 7r+ K -

K+Kpp "Y7 ~'f

~+#e+ ee + p,~: ~u'#

Confidencelevel (MeV/c)

+31 ) %

( 8.1 4. 2.4)% %

2321

21.8 % ( 9.3 ~ 3.3) x 1o- 4 < 1.2 x 10- 3 < 3.8 x 10- 3

~(2S) q~

90% 90% 90%

seen < < < < < < < < <

[hhh]

J/~(1S)~ +

[hhh] < 8.2

x 10- s

90%

-

J/'~,(1S)Tr+Tr+~r -

[hhh] < [hhh] < [hhh] <

x 10- 4 x 10. 3 x 10- 3

90% 90% 90%

-

D*(2010)+D 0

B0), the LEP Bs0 pro-

The first four were evaluated using B(b ~

1.7 2.1 1.0 1.5 2.1 5.9 5.9 1.48 7

159o 1788 1735

1122 x 10- 4 x 10- 4 x 10- 3 • 10- 3 x 10- 4 x 10- 5 x 10- 5 x 10- 4 x 10 - 4

Lepton Family number (LF) violating A B = 1 weak neutral current ( B 1 ) B1 < 2.0 x B1 < 5.4 x LF lee] < 6.1 x B1 < 5.4 x

98% 90% 90% 90% 90% 90% 90% 90% 90%

1122 2861 2655 2628 2660 2639 2515 2685 2588

90% 90% 90% 90%

2682 2864 2864

modes or modes 10 - 6 10 - 5 10 - 6 10 - 3

--

P Confidencelevel (MeV/c)

J/~(1S)s

J/~(15)a1(1260 )

These branching fractions all scale with B(b ~

Fraction ( r i / r ) (5.2+~:~) x 10- 5 5.7 1.2 6.2

46

Meson SummaryTable

II

II

M sor,,s iG(jPC ) = 0+(0- +)

Massm=2979.8• Full width F = 13"~+3.8 MeV ~-3.2 RC(I$) DECAY MODES

(S=1.9)

Confidence level

P (MeV/c)

(4.1 (2.6 (2.o (8.5 (?.1

K*(892) ~ K - ~r+ + c.c. K*(892)K*(892) q~ a0(980) ~ a2(1320) ~

K*(892)K+ f2 (1270)'r/

c.c.

Cd(d

• • • • •

% % % x 10 - 3 x 10 - 3

1319 1275 1273 1193 1086

< 2

%

90%

1323

< 2 < 1.28

% %

90% 90%

1193 1307

< t.1

%

90%

1142

< 3.1

X 10 - 3

90%

1268

Decays into stable hadrons KK~r

%

1378

%

1425

~77FTr

(5.5 • (4.9 •

~+ ~ - K + K -

(2.0 +0.7~ _0.6 ) o/ /o

2(K + K - )

(2.1 •

1342

%

lO53

2(/r+Ir -) p~ KK'q

(1.2 • (1.2 • < 3,1

% x 10 - 3 %

90%

1457 1157 1262

~r+~r-p~

< 1.2 < 2

% x 10- 3

90% 90%

1023 987

AA

Radiative decays (3.0 •

71'

I J/d/(1S)I

• 10 - 4

1365

x 10 - 4

1114

w fl (1420)

6.8 •

x 10 - 4

1062

• 10 - 4

--(1530)-_-=+

6.5 • 5.9 •

1320 597

p K-X(1385) ~

5.1 •

Ld~ 0

4.2 • 3.3 • 3.2 •

r f0(980)

-(153o)O-O

x 10- 4

1489

~v'(958) f0(980)

~d(958) p#~

J/@(1S) DECAY MODES

Fraction ( r i / r )

hadrons

(87.7 •

)%

virtual')' --* hadrons e+ e/~+ll~--

07.0 • (5.93• (5.88•

)% % %

Decays i n v o l v i n g h a d r o n i c p~

1.27• p0 ~r0

4.2 •

p (MeV/c) -1548 1545

%

1449 1449

1.09• 0.22) % 8,5 • x 10 - 3

CL=90%

X 10 -3

CL=90%

588

K*(892)~

<

5

x 10 - 4

CL=90%

1263

~ f2(1270)

<

3.7

x 10 - 4

CL=90%

1036

PPP

<

3.1

x 10 - 4

CL=90% CL=90%

779 946 1003

~

<

2,5

x 10 - 4

<

2.2

x 10 - 4

CL-90%

Z(1385)0A

<

2

x 10 - 4

CL=90%

911

.4(1232)+~ xo~ @=o

<

1

x 10- 4

CL=90%

1100

<

9

x 10- 5

CL=90%

<

6.8

x 10 - 6

CL=90%

1032 1377

Decays into stable hadrons 2(,K+ ~ - ) , a -0

3,37•

%

1496

3(.;,r + .a-- ) .K0 7r+ ~ - 7r0

2.9 +0.6 ) %

7r+ Tr-~rO K + K -

1.20• 9.0 •

% ) • 10 - 3

1433 1533 1368

2(~+ 7r-) 3(~ + ~-)

7.2 6.1 6,0 4.0 4.0

• • • • •

) ) ) ) )

#nTr +/F--

4

•

) x 10 - 3

1.50• 0,20} %

xo~o

2(:,r+~r-) K+ K -

p~Tr+r-~r 0 P~ PP~I p#~r-

4.2 • 3.8 • 3.4 •

x 10 -3 x 10 - 3 • 10 - 3

1371

I('+~T-

A X + c.c.

3.0 • 2.9 •

x 10- 3

1436 1299

• 10 -3

1210

2.3 • 2.04• 1,9 • 4.8 •

x 10 - 3

1299 969 1268

r

1.60•

X 10- 3

,~(1232)++ ~ r -

1.6 •

) X 10- 3

1.58•

• 10- 3

@KF

1.48•

X 10- 3

@fo(1710) ~ @KK p~w -4(1232) ++ ~ ( 1 2 3 2 ) - Z'(1385)- ~(1385) + (or c.c.) p~/(958) ~f~(1525)

3.6 •

) • 10- 4

1.30•

X 10- 3

1.10• 1.03• 9 • 8 •

• 10 - 3 x 10 - 3 ) x 10 - 4 ) x 10 - 4

lee]

[iii]

AA

K+K AATr o

B78 1318 1030 1394

5=1.3

5=1.7 S:2.7

1179 875 769 938 692 596 871

CL=90% CL=90%

~(144o) -~ ~ ~f~(z525)

pK-~

X 10 - 3 • 10- 3 • 10- 4

) x 10 - 5 x 10- 3 x 10 - 3

1271 1283 527 1263 1159

x 10 - 3

1098 1373

K • K O~T b1(1235) 0 ~r0 ~ K * ( 8 9 2 ) K + c.c. ~KK ~f0(1710)-~ ~ K K

x 10- 4 ) • 10- 4

1032 1398 1279

2.9

1005

[ee] [eel

S=1.1

x 10- 4

3.0

x 10- 3 x 10 - 3

b~(1235)• 9

6O8 857

<

• 10- 3

Ld ~-0 ~-0

• 10- 4 • 10 - 4 • 10 - 4

<

5.3 • 5.0 •

~ f2(1270) K*(892)~ + r ~ K * ( 8 9 2 ) K + c.c. K + K* (892)- + c.c. K~ ~ + c.c. K1(1400) • K m

1192 1182

K~(1430)~ K~(1430) 0

x i0 - 3 X 10- 3

:r

(~p71-+7f-

S=1.9

K1(1270) • K m

7.2 • 4.3 • 6.7 •

Cd'K+ "K-F?r

x 10 - 4 x 10 - 4

<

1125 1392 1435 1143

a2(1320)p

645 1447

K K ~ ( 1 4 3 0 ) + c.c.

[eel <

resonances ) x 10 - 3

S=1.4

4,5 i l . 5 4.3 4.0

a2(1320)• ~m

p-~Tr+~r -

Scale factor/ Confidence level

x 10 - 4

1.05+0.18) x 10- 4

7r+ Tr- K + K K -K Tr

Mass m = 3096.87 • 0.04 MeV Full width F = 87 • 5 keY Fee = 5.26 • 0.37 key

3,1 • 2.6 • 1,93• 1.67• 1.4 •

r f1(1285)

4(~+~-)~ ~

IG(jPC) = 0-(1 - - )

x 10 - 4 • 10 - 4

3.2 •

[eq

X(1385)-X + (or c.c.)

Decays Involving hadmnic resonances pp

8.0 • 7.2 •

[ee]

r162

Fraction ( r i / r )

r/(958)~r?r

r ~+ 7c-

p~r ~

A~- ~+ (or c.c.)

[ee]

pK-A

2(K + K - ) o

Ko~Ko,

10 - 3 10- 3 10- 3 10 - 3 10 - 3

1345

S=L3

1407 1440 1107 1517 1466 1106

1,27•

• 10 - 3

3.1 • 2.3 •

)xlO -3 ) x 10 - 3

212• 2.09•

• 10 - 3 x 10 - 3

1232 948

2.00• 2,2 • 1,8 • 1,30• 1.09• 1.06• 8.9 • 7.0 •

x 10 - 3 ) x 10 - 3 ) x 10 - 3 x 10 - 3 x 10 - 3 • 10- 3 ) x 10- 4 ) x 10- 4

1174 1231 81B 1074 1176 945

2.9 • 2,37• 2.2 • 1,47• 1.88•

) • • ) • x x

1.5 5,2

0 0 KsK 5

x x • x •

S=1.9

S=1.8

S=I.1

876 1131

10 - 4 10 - 4 10 - 4 10 - 4 10 - 4

x 10 - 4

x 10 - 6

992 1320 1033

820 1468 998 1542 1466 CL=90% CL=90%

1032 1466

Radiative decays

~nr 77r+ ;r

21r0

1'rpr 7r 3'7/(1440)--* 7KKTr ? r / ( 1 4 4 0 ) --~ 1 " 7 p 0

[p]

1.3 • 8.3 •

)%

6.1 •

) x 10- 3

9.1 •

) x lO-4

-

6.4 • 3,0 •

) x 10- 5 ) x 10 - 4

--~ 7 1 r + ~ r -

4.5 • 6.2 •

) x 10- 3 ) x 10- 4

7 2~+ 2rr-

4,31• 2.8 •

) X I0 - 3

1" K + K - ~ r + ~ -

2.1 4-0,6 ) • 10- 3

1' f4(2050)

2.7 •

1'cdw

1.59+0.33) • 10- 3

,77/(1440) - ~

1'Tt~•

7PP 7~(1870)

~n'(958)

116

) x 10- 3

1518 1487 1223 1223 1343

x 10 - 3

) x 10- 3

S=1.9

1400 1517 874 1337

47

Meson SummaryTable 7pOp ~

"},q(1440) ~ 3' f2(1270)

1.7:50.4 ) x 10- 3 1.38:50.14) x 10- 3

"}'f0(1710) ~

8.5

7KK

")'f1(1420) --~ 7 K K * 7 f1(1285)

~r+~ -

~f1(1510)-~

+~:2 ) • lO-4

8.6 +0.8 8.3 +1.5 6.1:50.9 4.5:51.2

) x ) • )x ) •

t~:~

7 f2(1950) --~ 7 K*(B92)K*(892) 7 K*(a92)K*(892)

7 . 0 : 5 2 . 2 ) x 10- 4

~A7 3~ 7 fJ(2220) 7 f J ( 2 2 2 0 ) -~ ~fj(2220)--~

7** 7KK

7fJ(2220)--,

"TPP

~fo(15oo)

lO75 1500 1220 1283

1173

) X 10 - 4

4.0:51,3 ) x 4.0 +1.2 ) x 3.8 +1,0 ) x 2.9 -I-0.6 ) x 1.3 +0.9 ) x 3.9 +1.3 ) x 7.9 x 5 x < 1.3 x < 5.5 x > 2.50 x ( 8 :54 ) x ( 8.1 +3.0 ) x ( 1.5 4-0.8 )x

'7"7

s=1.2

10- 3 10- 4 10- 4 10- 4 10- 4 10- 5 10- 4 10- 4 10- 4 10 -5 10 -3 10- 5 1o- 5 10 -5

2(/r+ 7r- )

-

p0 ~F+ ,n._

CL=90% CL--90% CL=90% CL=90% CL-99.9%

1166 1232 834 1048 1546 1107 1548 1074 1548 -

K + K * (892) 0 ;r- + c.c.

7r+ , K+K K+K-K+K o o KsK s P~ J / ' ~ ( l S ) 7r+ * - ~r0 K ~ K + , - + c.c.

Scale factor/ p Confidencelevel (MeV/c)

Fraction ( r i / r )

XC2(1P) DECAY MODES

3(.+ ~-) S=2.1

0+(2 + +)

Full width F = 2.00 • 0.18 MeV

~+.-K+K

Hadronic decays ( 1.2 + 0 3 (10 :54 9.2 +2.2 7 :k4 4.8 ~ 2 . 8 1.4 + 0 . 6 2.0 +0.8 1.52+0.25 8.1 + 1 . 9 1.5 + 0 . 4 6.1 +2.3 < <

9.8 + 1 . 0 1.5 1.06

% x 10 - 3 x 10- 3 x 10- 3 • 10 - 3 x 10 - 3 x 10- 3 x 10- 3 x 10- 4 • 10 - 3 x 10- 4

x I0 - 5 % x I0 -3

S=2.2 S=2.0

S=1.5

1751 1656 1707 1683 1601 1410 1773

1708

1510

CL=90% CL=90%

185

Radiative decays

-rJ/~(lS)

<( 5.7 +0.8 )x 10 -4 ( 8.8 + 1 , 4 ) x 10 - 3

,),e+ e -

iG(jPC) = Mass m = 3556.18 ~: 0.13 MeV

10 -4

4m7

7q(2225) 7r/(1760) --* 7p~ p~ ,),~r0 ~p~*+,-

1223 1286

10- 4 10 - 4 10-4

7f~(1525)

"),p~

S=1.3

1184

(13.5 +1.1 ) % ( 1.6 +0.5 ) • 10- 4

77

430 1778

I e ( J PC) = 0 - ( 1 - - )

I Xco(1P) I

IG(JPC)=

0+(0 + +)

Mass m = 3685.96 + 0,09 M e V Full width F = 2 7 7 •

Mass m -- 3415.0 • 0.8 M e V Full width r = 14 Q+2.6 M e V "--2.3 Xc0(1P) DECAY MODES

2(.+~-) .+.-K+K

poct+.3(.+.

-

- )

K + K * (892) 0 7 r - + C.C. ;T:5*--

K+K 7r+ , - p - ~ K+K-K+K K so K o$ K~

-

Hadronic decays (2.0 +0.9 ) (1.8 + 0 . 6 ) (1.6 +0.5 ) (1.24+o.22) (1.2 +0.4 (5.0 +0.7 (5.9 + 0 . 9 (1.8 +0.9 (2.1 4-0.5 (2.0 +0.6

77

1679 1580 1608 1633 1522 1702 1635 1320

DECAY MODES

Fraction

hadrons v i r t u a l 7 --~ hadrons e+e-

x 10- 4

S=2.1

Radiative decays (6.6:51.8 (2.7 :bl.9

x 10- 3 x 10- 4

1427

303 1708

J/O(1S)*~

~T0

J/~(is),

3(:T+ 7 r - ) :r 2(7r+ :rr-) :rr0 wf2(1270) pa2(1320)

. + IT- K + K K*(B92)K~,(1430) 0 K1(1270) + K:F

0.14 M e V

2(*+* -)

~r+ Tr- K + K pO~r+ , K+K-*(892)~ K~ K + *,+,-p~

- + c.c.

K+K -

<

+ r

2(7r + ~r-)

Fraction ( r i / r ) H a d r o n l c decays 6.3•

3(.+~-)

K+'K*(892)~ bl~ 7r:F

0.12 M e V

Scale factor

p (MeV/c)

pO,+,~P

3(~+ ~-)

5.6+2.6) 4.9+1.2) 3.9+3.5) 3.2• 2.5+0.8)

x x • • • •

10- 3 10- 3 10- 3 10- 3 10- 3 10- 3

5.4+2.1) 4.2:5L9) 8.2+1.3) 2.1

• x • x

10- 4 10- 4 10 - 5 10- 3

~pTr ~

2.2 1.1

1683 1727 1632 1659 1576

-

1381

K + K- ,o 1483

R a d i a t i v e decays

(27.3+1.6) %

K+K

, + Tr-Tf 0 pTr 7r+ ~TA-A KI(1400)+ K:F

1.2

389

(98.10:5/:0.30) %

( 2.9 +0.4 ) % ( 8.8 + 1 . 3 ) x 10 - 3 (1.o3+o.35) %

(55 (23.1 (31.0 (18.2 ( 2.7 ( 9.7

J/~(]S)~+ ~-

K + K * ( 8 9 2 ) - + c.c. @f~(1525)

Scale factor/ p Confidence level (MeV/c)

(ri/r)

Decays into J/'@(15)and J / ~)(1S) anything J/~b(15) neutrals

IG(jPC) = 0+(1 + +)

XCl(1P) DECAY MODES

?J/~(1S)

r

J/~'(1S)* 0

(2.2 + 1 3

Full width r = 0.88 •

+

S-1.6

CL=90%

Mass m = 3510.51 •

~+,-

S=2.7 S=1.9

x 10- 4 x 10 - 4

I Xcl(1P)I

K+K-K+K p-~

% % % % % x 10 - 3 x 10 - 3 x i0 -3 x I0 -3 x 10- 3

(9 -t-5 < 7.1

P~

7J/~)(15)

Scale factor/ p Confidencelevel (MeV/c)

Fraction ( r i / r )

+ c.c.

(S=1.1)

Fee = 2.12 • 0,18 keV

1843 1840

anything

+5 +2.3 +2.8 • +0.4 +2.1

% % % % % x 10- 4

Hadronic decays ( 3.5 +1.6 ) x lO - 3 ( 3.0 + 0 . 8 ) x lO - 3 < 1.7 x 10 - 4 < 2.3 x 10- 4 ( 1.6 + 0 . 4 ) x 10 - 3 < 1.2 x 10 - 4

477 481

S=1.6

1746 1799 CL=90% CL=90% 1726 CL=90%

1.00+0.28) x 10- 3 8.0 • x 10 - 4 6.7 +2.5 X 10- 4 5.2 •

1491 1673

x 10 - 4

X 10 - 4 +1.5 X 10- 4 • x 10- 4 + 1 . 0 , X 10 - 4 x 10 - 4 +0.5 +0.7 , x 10 - 4 x 10- 5 +5 • 10-5 < ) • 10- 5 (8 +5 • 10 - 4 < 4 • 10- 4 < 3.1 x 10- 4 < 2 x 10-5 < 2.96 x 10-5 < 5.4 x 10-5 < 4.5

4.5 4.2 1.9 1.5 1.4 1.0 8 8.3

200 527

+1.0

1817

CL=90% CL--90% CL=90% CL=90% CL=90% CL=90% CL=90%

1751 1586 1774 1543 1776 1830 1760 1838 1467 1285 1754 1698

48

Meson SummaryTable Radiative

3`Xco(1P)

decays

( 9.3 •

3`Xcl(1P)

)%

3`r/c(15)

( e.7 +0.B )% ( 7.8 • )% ( 2.8 4-0.6 ) x 10-3

3`~/'(958)

( 1,5 •

3`Xc2(1P)

3'7 3'7 3'7/(1440) ----, 7 K K ~

I r

< < <

) x 10- 4

9

x 10- 5

1.6 1.2

x 10- 4 x 10- 4

~($'rto) DECAY MODES

Fraction ( l ' i / r )

DD e+ e-

dominant (1.12•

u#}I

II

..~

IG(j Pc) = Mass m = 9460.30 + 0,26 MeV Full width F = 52.5 • 1.8 keV Fee = 1,32 4- 0.05 keY

T+T

Scale factor

P (MeV/c)

1.2

242 1885

x 10- 5

:(:PC) = o-(1 - - )

@(4040) DECAY MODES

Fraction ( r i / r )

e+e D0D ~ D * (2007) 0 9 0 + C.C. D * (2007) 0 D* (2007) 0

(1.4• seen seen seen

p (MeV/c)

x 10- 5

2020 777 578 232

IG(jPC)= 0 - ( I

-

J/@(1S)anything

Hadronlc decays (1.1 •

< 5 < 1.84

) x x x x x x

10- 3 10- 4 10- 4 10 - 4 10 - 4 10- 5

Fraction ( r i / r )

- -)

p ( M eV/c)

• 10- 6

IG(JPC)=

2079

0-(1

- -)

Mass m = 4415 4- 6 MeV

Full width F = 4 3 4 - 1 5 M e V Fee = 0.47 • 0.10 keY

3` 7r0 ~r0

(6.3 • (1.7 •

) x 10- 5 ) x 10- 5

3` 2 h + 2 h -

(7.0 •

) x lO-4

3`3h + 3 h 3`4h+4h -

3`x + 7r-

K + K-

3`2~r+ 27r -

7 37r+ 37r-

3`2~r+ 27r-K+ K-

(5.4 (7.4 (2.9 (2.5 (2.5 (2.4 (1.5 (4 (2.0 < 1.3 < 3.5 < 1.4

3' f2(1270)

(lO•

DECAY MODES

4730 4729

p~ 1T0/r+~T -

3'f~(1525)

e+e -

had rons e+ e -

4384

(2.38• 0.11) % (2.48 • 0.06) %

< 2 < 5 < 5

3'7f(958) 77/

@(4160) DECAY MODES

r

12 n7+0.14~ ,/,o , ..._0.161

p/r ~T+ / r K + K-

7~r+~r- p~ 7 2~r+ 27r- p~ 3`2K+2K -

Mass m = 4159:5 20 MeV Full width F = 78 + 20 MeV Fee = 0.77 :I: 0.23 keY

I •(4415) Fi/] I

P Confidencelevel (MeV/c)

(ri/r)

90% 90% 90%

90% 90%

4223 4698 4728 4704 4636 - -

Radiative decays

Full width F = 52 4- 10 MeV Fee = 0.75 4- 0.15 key

I

(S = 3.3)

Fraction

e+ e /~+/~-

Mass rn = 4040 4- 10 MeV

I ~b(4160) [/J/]

0-(1 - -)

= 0-(1 - - )

Mass m = 3769.9 4- 2,5 MeV ( S = 1 . 8 ) Full width F = 2 3 . 6 4 - 2 . 7 M e V ( 5 = 1 . 1 ) Fee = 0 . 2 6 • (S=1.2)

Ir

II T(16) DECAY MODES

IG(jPC)

I

CL=90% CL=90% CL=90%

261 171 127 639 1719 1802 1843 1569

iS=1.8)

Fraction

(rdr)

dominant (1.1• x 10- 5

p (MeV/c)

3`7(1440)

< < < < < <

• ) • 10- 4 • X 10- 4 .4-0.9 x 10- 4 • X 10- 4 • x 10- 4 -I-1.2 x 10- 4 • x 10- 4 +6 x 10- 5 • x 10- 5 x 10- 3 x 10- 4 x 10- 4

(8 4-4 8.2 2.6 2

3`fo(1710)-~ 3 ' K K 3' fo(2200) --* 3' K + K 1.5 3' fJ(2220) --* 3"K+K3 3`T/(2225)--~ 7 ~ 3 3`X X = pseudoscalar with m< 7.2 GeV) 3`XX < 1 X X = vectors with m< 3.1 GeV) I Xb0(1P)

[kkk] I

4720 4703 4679

90% 90% 90%

4686 4720 4703 4658 4604 4563 4601 4682 4714 4607

x 10- 5 x 10- 5 x 10- 4 x 10- 4 x 10- 5 X 10- 3 x 10- 5

90% 90% 90% 90% 90%

4644 4624 4576 4475 4469 4469

x 10- 3

90%

90%

/G(jPC) = 0+(0 + +) J needs confirmation.

Mass m = 9859.9 + 1.0 MeV

2207

Xb0(1P) DECAY MODES

Fraction

3` T ( I S )

<6%

I Xbl(1P) [kkk] I

(Fi/F)

90%

391

IG(jPC)

= 0 + ( 1 + +) J needs confirmation.

Mass m = 9892.7 -I- 0.6 MeV

(S -- 1.1)

Xbl(1P) DECAY MODES

Fraction ( r f / r )

3` ? ' ( 1 5 )

(35•

I Xb2(1P) [k,k] I

P Confidencelevel (MeV/c)

%

p (MeV/c)

422

I6(jPC)

= 0+(2 + + ) J needs confirmation.

Massm= 9912.6+0.5 MeV

(S--1.1)

Xi~(1P) DECAY MODES

Fraction (Fi/F)

'7 T(IS)

(22•

%

p (MeV/c)

443

49

Meson Summary Table - ~

IG(J PC) =

0-(1 - -)

Mass m = 10.02326 • 0.00031 GeV Full width r- = 44 4- 7 keY Fee = 0.520 4- 0.032 keY "/(25) DECAYMODES

r+r

"YXb0(2P) P Confidencelevel (MeV/c)

Fraction ( r t / r )

T(lS)Tr+x T(1S)~r%r 0

(18.8:1:0.6 ) %

#+/~e+e T(1S)Tr~ T(1S)r I

J/~)(1S)anything

3'f0(1710) 7f~(1525) 3,f2(1270)

I Xb0(2P) [*kk] I

4686 5011 5012 531 127 4533

90% 90%

90%

90% 90% 90%

131 110 162 4866 4896 4931

Fraction ( r i / r )

BB non-BB

> 96 < 4 (2,8+0.7) (2.2+0.7) < 7.4 < 2.3 < 4 < 1.2 < 3.9

J/~b(3097)anything D *+anything + c.c. ~anything T(1S)anything T(1S)~+~ T(2S) ~T+7r-

(4.64.2.1) % (9 4.6 ) x l 0 -3

I Xbl(2P)

[kkk]

Xbl(2P)

210 746

?T(2S)

I X~(2p) [kkk] I

T(10860) DECAY MODES

Fraction (rilr)

e+e -

(2.8+o.7} x 10-6

95% 95%

90% 90% 90% 90% 90%

5290 5099 5240 1053

0-(1 - -)

p Scale factor (MeV/c)

Fraction (I-t/r)

IG(JPC) =

p (MeV/c) 5432

0-(i - -)

Mass m = 11.019 4- 0.008 GeV Full width r = 79 4- 16 MeV Fee = 0.130 4- 0.030 keY

23.5 4- 1.0 MeV

(21 +4 )% ( 8.5:1:1.3)%

~ T(I$)

% % x 10-5 x 10-3 % x 10-3 x 10-3 ;<10-4 • -4

I6(J PC) =

I T(11020)I

I6(jPC) = 0+(1 + + ) J needs confirmation. Mass m = 10,2552 4- 0.0005 GeV

DECAY MODES

P Confidencelevel (MeV/c)

p (MeV/c)

I

mxH(2p) -- mxbo(2P) :

S=1.1

Mass m = 10.865 4- 0,008 GeV (S = 1.1) Full width I- = 110 • 13 MeV Fee = 0.31 4- 0.07keY ( S = 1 . 3 )

Mass m = 10.2321 • 0.0006 GeV

")"T(2S) 3, T ( l S )

87 100 123

= 0-(1 - -)

1"(45) DECAY MODES

J needs confirmation.

Fraction ( r i / r )

S=1.3

Mass m = 10.5800 4- 0.0035 GeV Full width r = 14 4 - 5 M e V ( S = 1.7) Fee -- 0.248 4- 0.031 keY (S = 1.3)

I T(10860)I

IG(j PC) = 0+(0+ +)

X~(2P) DECAY MODES

IG(jPC)

or "/'(10580)

e+e-

Radiative decays ( 6.8 4.0.7 )% ( 7.0 =t=0.6 )% ( 3.8 =I=0.6 )% < 5.9 x 10-4 < 5.3 x 10-4 < 2.41 x 10 -4

"TXbl(1P) "TXb2(1P) 7Xbo(1P)

I T(4s) I

475 480

( 9.0 ~:0.8 )% ( 1.7:1=1.6 )% (1.31:1:0.21) % (1.18~:0.20) % < 1.1 x 10-3 < 2 x 10-3 < 6 x 10-3

-

Radiative decays (11.4 4.0,8 ) % (11.3 4.0,6 )% ( 5.4 4.0,6 )%

~/Xb2(2P) "YXbl(2P)

1.5 1.3

229 764

T(11020) DECAY MODES

Fraction

e+ e-

(1.6•

(r~ir) x 10-6

p (MeV/c) 5509

NOTES

IG(jPC)

= 0+(2 + + ) J needs confirmation. Mass m = 10.2685 4- 0.0004 GeV mxa2(2P) - mxH(2p) = 13.5 4- 0.6 MeV

In this Summary Table:

Xb2(2P) DECAYMODES

Fraction (ri/r)

p ( MeV/c)

T(25) ~r T ( I S )

(16.24.2.4) % (7.1• %

242

IG(J PC) =

776

A decay momentum p is given for each decay mode. For a 2-body decay, p is the momentum of each decay product in the rest frame of the decaying particle. For a 3-or-more-body decay, p is the largest momentum any of the products can have in this frame.

0-(1 --)

Mass m = 10.3552 4- 0.0005 GeV Full width r = 26.3 4- 3.5 keV Scale factor/ p Confidencelevel (MeV/c)

1"(35) DECAY MODES

Fraction ( r / / r )

T(2S)anything T(2$)~+x T(2S)~r~ ~ T(25)'~')" T(1S)~ + ~rT(15)lr0~ 0 T(1S)T/ /z+/~e+ e-

(10.6 4-0.8 )% ( 2.8 • )% (2.004.0.32) % ( 5.0 4-0.7 )% ( 4,48-!-0.21} % (2.064.0.28) % < 2.2 x 10-3 (1.814.0.17) % seen

When a quantity has "(S . . . . )" to its right, the error on the quantity has been enlarged by the "scale factor" S, defined as S = ~ 1), where N is the number of measurements used in calculating the quantity. We do this when S > i, which often indicates that the measurements are inconsistent. When S > 1.25, we also show in the Particle Listings an ideogram of the measurements. For more about S, see the Introduction.

S=2.2

CL=90%

296 177 190 327 814 816 5177 5177

[a] See the "Note on ~r+ ~ t ~- L,3" and K • --, g• u3' Form Factors" in the 7t• Particle Listings for definitions and details.

r(e+Ve)/r(~+~.)

[b] Measurements of always include decays with 3"s, and measurements of r(e + ='e'r) and r ( # + u~3,) never include low-energy ?'s. Therefore, since no clean separation is possible, we consider the modes with 3"s to be subreactions of the modes without them, and let [r(e + re)

+ r(~+~.)]Irtota, =

100%.

[c] See the 7t• Particle Listings for the energy limits used in this measurement; low-energy 7's are not included.

50

Meson Summary Table [d] Derived from an analysis of neutrino-oscillation experiments. [e] Astrophysical and cosmological arguments give limits of order 10-13; see the ~r~ Particle Listings. [f] See the "Note on the Decay Width F(T/ -~ "f~')" in our 1994 edition, Phys. Rev. DS0, 1 August 1994, Part I, p. 1451. [E] C parity forbids this to occur as a single-photon process. [h] See the "Note on scalar mesons" in the fo(1370) Particle Listings. The interpretation of this entry as a particle is controversial. [f] See the "Note on p(770)" in the p(770) Particle Listings. [./] The e+ e- branching fraction is from e+ e - --~ ~r+ 7r- experiments only. The ~ p interference is then due to ~ p mixing only, and is expected to be small. If e# universality holds, r(p 0 --, /~+#-) = F(p0 --~ e+e - ) • 0.99785. [k] See the "Note on scalar mesons" in the f0(1370) Particle Listings. [f] See the "Note on a1(1260)" in the a1(1260 ) Particle Listings. [m] This is only an educated guess; the error given is larger than the error on the average of the published values. See the Particle Listings for details. In] See the "Note on the f1(1420)" in the fl(1440) Particle Listings. [o] See also the ~(1650) Particle Listings. [p] See the "Note on the 7(1440)" in the 7(1440) Particle Listings. [q] See the "Note on the p(1450) and the p(1700)" in the p(1700) Particle Listings. [r] See the "Note on non-q~ mesons" in the Particle Listings (see the index for the page number). Is] See also the ~(1420) Particle Listings. It] See the "Note on fo(1710)" in the fo(1710) Particle Listings. [u] See the note in the K :I: Particle Listings. [v] The definition of the slope parameter Eof the K --* 3~r Dalitz plot is as follows (see also "Note on Dalitz Plot Parameters for K --* 3~r Decays" in the K - Particle Listings):

IMI =

+ g(s

- So)/m2r + + . . . .

[w] For more details and definitions of parameters see the Particle Listings. [x] Most of this radiative mode, the low-momentum 3' part, is also included in the parent mode listed without 3"s. [y] See the K + Particle Listings for the energy limits used in this measurement. [z] Direct-emission branching fraction. [aa] Structure-dependent part.

[bb] Derived from measured values of ~+_, ~o0, 171, Im~o - m~l, and TK~, as described in the introduction to "Tests of Conservation Laws."

[cc] The CP-violation parameters are defined as follows (see also "Note on CP Violation in K s --, 3~r" and "Note on CP Violation in K ~ Decay" in the Particle Listings):

A(K 0 ..-* ~r+ Tr-) 7+-= 700 =

~=

17+_]e'~+17Dolei~|

-

A(KO S-~ ~+=_)

A(Ko ~ ~%o) A(K o _~ ~%0)

r(K o -~ ~ - t + v ) r ( K ~ -~ ~ - t + v ) I-(Ko ~

Im(7+_o) 2 =

~ + ~'

[ft'] ct/~ is derived from ]7oo/r/+_l measurements using theoretical input on phases.

[EE] See the K ~ Particle Listings for the energy limits used in this measurement.

[hh] Allowed by higher-order electroweak interactions. [ii] Violates CP in leading order. Test of direct CP violation since the indirect CP-violating and CP-conserving contributions are expected to be suppressed. ~ ] See the "Note on fo(1370)" in the f0(1370) Particle Listings and in the 1994 edition. [kk] See the note in the L(1770) Particle Listings in Reviews of Modern Physics 56 No. 2 Pt. I1 (1984), p. $200. See also the "Note on K2(1770 ) and the/(2(1820)" in the K2(1770 ) Particle Listings. [If] See the "Note on K2(1770 ) and the K2(1820)" in the K2(1770 ) Particle Listings. This result applies to Z ~ ---* cs decays only. Here t + is an average (not [ram] a sum) of e+ and #+ decays. [nn] This is a weighted average of D :1: (44%) and D O (56%) branching fractions. See "D+andD ~ -~ (7/anything) / (total D + and DO) '' under "D + Branching Ratios" in the Particle Listings. [oo] This value averages the e+ and #+ branching fractions, after making a small phase-space adjustment to the/~+ fraction to be able to use it as an e+ fraction; hence our t + here is really an e+, [pp] An t indicates an e or a/~ mode, not a sum over these modes. [qq] The branching fraction for this mode may differ from the sum of the submodes that contribute to it, due to interference effects. See the relevant papers in the Particle Listings. [rr] The two experiments measuring this fraction are in serious disagreement. See the Particle Listings. [ss] This mode is not a useful test for a A C = I weak neutral current because both quarks must change flavor in this decay. [tt] This D~ O limit is inferred from the D~ ~ mixing ratio F(K+Tr - (via D~ / F(K-7r +) near the end of the D o Listings. [uu] The experiments on the division of this charge mode amongst its submodes disagree, and the submode branching fractions here add up to considerably more than the charged-mode fraction. [vv] However, these upper limits are in serious disagreement with values obtained in another experiment. [ww] For now, we average together measurements of the X e+ r,e and X/~+ vp branching fractions. This is the average, not the sum. [xx] This branching fraction includes all the decay modes of the final-state resonance. Lvy] This value includes only K + K - decays of the f0(1710), because branching fractions of this resonance are not known. [zz] This value includes only 7r+ 7r- decays of the fo(]500), because branching fractions of this resonance are not known. [aaa] B ~ and B ~ contributions not separated. Limit is on weighted average of the two decay rates.

[bbb] These values are model dependent. See 'Note on Sernileptonic Decays' -

c

-

2~ ~

r(K o -~ l r + l - v ) + r ( K ~ -~ ~r+t-~) ' ~+~-~rO)CP viol

r(K o _., ~+~-~o)

im(~/0oo)2 = r ( K ~ - ~ ~%r%r ~ r(KiO __, ~o~o~0) where for the last two relations CPT is assumed valid, Le., Re(7+_o) 0 and Re(700o) -~ 0. [dd] See the K 0 Particle Listings for the energy limits used in this measurement. [ee] The value is for the sum of the charge states or particle/antiparticle states indicated.

in the B + Particle Listings.

[ccc] D** stands for the sum of the 0(1 1P1), 0(1 3Po), O(13p1), O(1 3P2), s

and 0(2151) resonances.

[ddd] D(*)D(*) stands for the sum of D ' D * , D ' D , DD*, and D ~ . [eee] Inclusive branching fractions have a multiplicity definition and can be greater than 100%. [fff] Dj represents an unresolved mixture of pseudoscalar and tensor D** (Pwave) states. [g&E] Not a pure measurement. See note at head of B 0 Decay Modes.

[hhh] Not a pure branching ratio, it is the fraction ( F i / F ) x B ( ~ --, Be). [iii] Includes p~Tr + 7r-~ and excludes PPT, pp~u, p-~'. [jjj] jPC known by production in e+e - via single photon annihilation. I (3 is not known; interpretation of this state as a single resonance is unclear because of the expectation of substantial threshold effects in this energy region. [kkk] Spectroscopic labeling for these states is theoretical, pending experimental information.

51

Meson Summary Table See also the table of suggested q~ quark-model assignments in the Quark Model section. 9 Indicates particles that appear in the preceding Meson Summary Table. We do not regard the other entries as being established. Indicates that the value of J given is preferred, but needs confirmation. LIGHT UNFLAVORED (s = c =

B

= o)

IG( J PC) 9 ~• 9

~0

9 9

6(400-1200)

p(770) 9 w(782) 9

i - (0-) 1-(0 - +) 0+(0 - +) 0+(0 + +)

9

I+(i--)

7r2(1670) ~(1680) p3(1690)

9 K*(892)

X(lrrS)

9 ao(980) 9 @(1020)

1-(0 + + ) 0-(i - - ) 0-(1 + -)

a2(1750)

9 9

~(1800) 6(1810) ~3(1850) 7/2(1870)

1-(2 + + ) o+(o - +) 1-(? 1-(o 0+(2 o-(3

- +) - +)

+ +) - -) 0+(2 - +)

9 bi(1235)

I+(I

9 a1(1260) 9 6(1270) 9 6(1285) 9 fl(1295)

I-(i 0+(2 + +)

X(1910)

0+(77+)

6(1950)

0+(2 + + )

o+(1 + +)

x(2ooo)

1-(? ?+)

9 ~(1300)

a2(1320) 9 ~(1370) h~(1380) ~i(1400) 9 6(1420) 9 w(1420) 9

0+(0 1-(0 1-(2 0+(0

+ +

+) +) +) +)

?--(i + -)

9 .(144o)

1--(1 0+(1 0-(1 0+(2 0+(0

9 ao(1450)

1-(o++)

9 p(1450)

1+(1 - - ) 0+(0 + +) 0+(1 + +) 0+(2 + +) 0+(2 + +) 1-(1 - +) 2+(2 + +) 1+(1++) o+(2 + +) 0+(2 - +) o-(1 - - ) o-(F-) 1-(2 + + )

6(143o)

9 6(1500)

6(1510) 9

f~(1525) 6(1565)

~1(1600) X(1600) a1(1640)

6(1640) 7/2(1645) 9 w(1650) x(165o)

a2(1660) 9 w3(1670)

0-(3

+ + -

-

+) +) -) +) +)

-)

1/2(0-) 1/2(0-) 1/2(0-) 1/2(0-)

o+(o + +)

7/(1760)

--) + +)

K+ K0 K~ K0L

9 fo(1710)

o+(o + +)

+

9

9

6(980)

hl(l170 )

1-(2 - +)

9 f2(2010) 6(2020) 9 a4(2040) 9 f4(2050) f0(2060) 7r2(2100) f2(2150) p(2150) f0(2200) fj(2220) 7/(2225) p3(2250) 9 f2(2300) f4(2300) 9 f2(2340) p5(2350) a6(2450) ~(2510) X(3250)

+) o+(o + +) 0+(2 +

1-(4 + + ) 0+(4 + +)

o+(o++) 1-(2 - +)

o+(2++) i+(i - -)

9

9

0+(6 + + )

??(???)

OTHER LIGHT UNFLAVORED (S = C = B = 0) e+e-(1100-2200) ??(1 - - ) NN(1100-3600) X(1900-3600)

1o(jPc)

1/2(1 +)

K~(1430) 9 K~(1430) K(1460) K2(1580) K(1630) K1(1650) 9 K*(1680) 9 K2(1770) 9 K;(1780) 9 /<2(1820) K(1830) K~(1950)

1/2(0 +)

K~(1980)

1/2(2 + )

K~(2045) K2(2250) /<3(2320) K;(2380) /<4(2500) K(3100)

1/2(4 +) 1/2(2-) 1/2(3 +) 1/2(5-) 1/2(4-) ??(???)

1/2(2 +) 1/2(0-) 1/2(7 ?) 1/2(1 + ) 1/2(1-) 1/2(2-) 1/2(3-) 1/2(2-) 1/2(0-) 1/2(0 + )

(c= • 9

D+ DO

1/2(0-) 1/2(0-)

9

D*(2007) ~

1/2(1-)

9 D*(2010) ~

1/2(1-)

9 D1(2420)0 D1(2420)• 9 B~(2460)~ 9 D~(2460)+

1/2(1 +) 1/2(7 ?) 1/2(2 + ) 1/2(2 +)

D*(2640)•

1/2(? 7)

CHARMED, STRANGE (c=s= • D~ 9 B; • 9

Ds1(2536)~ O,j(2573) ~

B*

1/2(1-)

B_~(5732)

?(77)

BOTTOM, STRANGE (B= •

S= TI)

9 8~

o(o-1

B;

0(1-) 7(7 7 )

i/2(2-)

CHARMED

9 9

ADMIXTURE

1/2(1 +) 1/2(1-)

9

9

9

*

/<1(1270) 9 K1(1400 ) 9 K*(1410)

9

B+ 1/2(0-) B~ 1/2(0-) 9 B ~ / B ~ ADMIXTURE 9 B•176 9

1/2(1-)

9

o+(o + +) 0+(2 + + or4 + + ) o+(o - +) 1+(3 -) 0+(2 + +) 0+(4 + +) o+(2 + +) 1+(5 - -) 1-(6 + + )

BOTTOM (B = =1=1)

C= e = 0 )

I(JP)

p(1700)

9 fl'(958)

9

Io ( j Pc) 0-(1 - - ) 1+(3 - - ) 1+(1 - -)

9 9 9

0-(1 - -) 0+(0 - +)

9

STRANGE (S= •

B;j(5850)

BOTTOM, CHARMED (e = c = • 9

B~

0(0-1 CC

9 ~/c(1S)

0+(0 - +)

9 JI%6(1S) 9 Xco(1P)

0-(1 - -) 0+(0 + +)

9 Cl(1P)

o77

hc(IP) 9

+)

?'(?") 0+(2 + +)

Xc2(1P)

7/c(25)

??(??+)

9 ~(2s)

o-(1 - - )

9 %6(3770)

0-(1 0-(2 O-(1 0-(i 0-(1

%6(3836)

9 %6(4040) 9 %6(4160) 9 %6(4415)

-

-) -) -) -) -)

b~

9 r(lS)

o-(1--)

9 Xbo(1P) 9 XbI(1P)

0+(0 + +) 0+(1 + +)

9 Xb2(1P)

0+(2 + o-(1--) 0+(0 * 0+(1 + 0+(2 +

9 r(2s) 9 Xbo(2P) 9 Xbl(2P) 9 Xb2(2P) 9 r(3s)

+) +) +) +)

o- (1 - - )

0(0-) 0(? 7)

9 r(4s)

o - (1 - - )

9 ?'(10860)

0-(i--)

0(1 +) 0(??)

9 T(11020)

0-(1--)

NON-q~ CANDIDATES NON-q~ CANDIDATES