2015-11-181 work report about b to vt run-hui li

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22/6/17 1 Work Report about B to VT Run-Hui Li

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Page 1: 2015-11-181 Work Report about B to VT Run-Hui Li

23/4/20 1

Work Report about B to VT

Run-Hui Li

Page 2: 2015-11-181 Work Report about B to VT Run-Hui Li

23/4/20 2

content

About tensor mesons Comparison of tensor and vector mesons Calculation in pQCD, wave functions and

the counting rules About our programs The preliminary results

Page 3: 2015-11-181 Work Report about B to VT Run-Hui Li

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Momentum definition

In the rest frame of B meson, the lightcone momentum of B, tensor and vector mesons are defined as

r22 and r3

2 are kept for the convenience of polarization definitions.

However, little momentum violation, so the terms which proportional to the r2 should be neglect to keep the momentum conservasion.

Page 4: 2015-11-181 Work Report about B to VT Run-Hui Li

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About tensor

JP=2+

5 polarization states with Jz=2,1,0,-1,-2 Nonet:

a2(1320),K2*(1430),f2(1270),f2

’(1525)

Isovector

Page 5: 2015-11-181 Work Report about B to VT Run-Hui Li

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Mixing between f2 and f2’

D.M. Li, H. Yu, and Q.X. Shen, JPG 27,807(2001)

PDG, PLB 667,1(2008).

Page 6: 2015-11-181 Work Report about B to VT Run-Hui Li

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Polarization tensor The spin-2 polarization tensor can be constructed

by the spin-1 polarization vector:

Page 7: 2015-11-181 Work Report about B to VT Run-Hui Li

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By defining a new polarization vector

the tensor wave function can be expressed as

The wave function of the vector meson is

v is the light cone direction opposite to the one along which the tensor meson moves.

Page 8: 2015-11-181 Work Report about B to VT Run-Hui Li

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Calculation in pQCD-----Start from the weak effective Hamiltonian

Page 9: 2015-11-181 Work Report about B to VT Run-Hui Li

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Page 10: 2015-11-181 Work Report about B to VT Run-Hui Li

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Calculation in pQCD

Page 11: 2015-11-181 Work Report about B to VT Run-Hui Li

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Topological Diagrams in pQCD Emission diagrams

Annihilation diagrams

Page 12: 2015-11-181 Work Report about B to VT Run-Hui Li

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Wave functions

B meson wave function Asymptotic form of vector meson wave function

Page 13: 2015-11-181 Work Report about B to VT Run-Hui Li

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Counting rules for B to VV Emission diagrams

Annihilation diagrams

Page 14: 2015-11-181 Work Report about B to VT Run-Hui Li

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Wave function of tensor

Hard to establish the similar counting rules

Page 15: 2015-11-181 Work Report about B to VT Run-Hui Li

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Functions for all the figures By inserting different operators in the diagrams, one can

obtain all the possible functions for the figures. ex. When the tensor and vector meson is longitudinally polarised, the

function for the (V-A)(V-A) operator of the factorizable emission diagram is

For one polarization case, there are 20 nozero such functions. 3 polarization cases, 60 nonzero functions.

The decay amplitude can be expressed by these 60 functions.

Page 16: 2015-11-181 Work Report about B to VT Run-Hui Li

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The expressions of the amplitude

For each F function, different operators may contribute.EX.

Tree

QCD penguin

Electroweak penguin

Page 17: 2015-11-181 Work Report about B to VT Run-Hui Li

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By collecting the contributed figures and judging the Wilson coefficients for each figure, one can obtain the expressions of the amplitude.

EX.

Page 18: 2015-11-181 Work Report about B to VT Run-Hui Li

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About the programs

The next step is to obtain the numerical values for each F function on the above page and get the numerical results for the amplitude.

Purpose of the designing Not only for B to VT, but also for B to AT,VA decays. For the B to VT decays, 62 channels. The number of the B to AT

decays are also large. In the purpose of making it easier from the B to VT to B to AT (or even repeat the B to VA calculations), I design a program to generate the decomposition of the amplitude expressions automatically.

For the same purpose, we make many modules, trying to separate the process-independent functions.

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About the programs

13 files About 6000 lines, except the Vegas module. After correcting all the bugs, the B to AT can be calculated

by substituting the 2 amplitude files and setting some parameters in Wilsoninitial.for file.

Page 20: 2015-11-181 Work Report about B to VT Run-Hui Li

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Some preliminary results

Large deviations from the experimental data. Perhaps there are still some bugs in the programs.

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Plans for solving the problems

Making use of the similarities of the tensor and vector mesons, check our formulas for the 60 F functions again to make sure that they are correct.

EX.

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For the bugs in the programs, maybe we can figure it out by comparing the data of similar channels, or by analyzing the data of each figure.

Doing some form factor calculation, compare the results with the pQCD results for form factors.