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2011 QCD and High Energy Interactions - Rencontres de Moriond ...

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The counterpart of the ground-state saturation approximation here is retaining the contribution<br />

of the lowest P-wave resonance in the sum; then each power of time <strong>de</strong>rivative amounts to the<br />

extra power of −¯ǫ, where ¯ǫ=MP −MB ≈0.4GeV.<br />

In fact, there are two families of the P-wave excitations of B mesons corresponding to spin<br />

, ... receive contributions<br />

of light <strong>de</strong>grees of freedom 3<br />

2<br />

or 1<br />

2 . The combinations µ2 π−µ 2 G , ρ3 D +ρ3 LS<br />

only from the 1<br />

3<br />

2-family, whereas the 2-family gives rise to µ2π +2µ2 G<br />

3 , ρ3 D−2ρ3 LS<br />

3 , etc. 7 (the transition<br />

amplitu<strong>de</strong> into the lowest 1<br />

2 P-state appears to be suppressed). Therefore, it makes sense to<br />

consi<strong>de</strong>r these two structures separately <strong>and</strong> approximate<br />

〈B| ¯b iDj(−iD0) k+1 <br />

iDl b|B〉 = ¯ǫ k 2ρ<br />

3/2<br />

3 D −ρ3LS + ¯ǫ<br />

9<br />

k ρ<br />

1/2<br />

3 D +ρ3 <br />

LS<br />

δjl (23)<br />

9<br />

〈B| ¯biDj(−iD0) k+1 iDlσjl b|B〉 = −¯ǫ k 2ρ<br />

3/2<br />

3 D −ρ3LS 3<br />

+ ¯ǫ k 2ρ<br />

1/2<br />

3 D +2ρ3LS . (24)<br />

3<br />

Note that assuming ¯ǫ 1/2 = ¯ǫ 3/2 = ¯ǫ implies ρ3 D ≃¯ǫµ2 π <strong>and</strong> −ρ3LS ≃¯ǫµ2 G ; the first relation seems to<br />

be satisfied by the preliminary values of µ 2 π <strong>and</strong> ρ3D extracted from experiment.<br />

This ground state saturation method can be exten<strong>de</strong>d also to higher dimensional operators<br />

in an obvious way. Furthermore, there is also the possibility for a refinement of the method by<br />

including more states asi<strong>de</strong> from the ground state. In this way a systematic approach can be<br />

constructed to obtain reliable estimates for the higher or<strong>de</strong>r matrix elements.<br />

3 Conclusion<br />

Evaluating the contributions appearing at or<strong>de</strong>r 1/m4 b quantitatively the impact on the <strong>de</strong>termination<br />

of Vcb is small <strong>and</strong> of the expected size. The <strong>de</strong>termination of Vcb makes use of the<br />

total rate which receives only small corrections. Inserting the numerics we get for<br />

the results<br />

<br />

<br />

δΓ<br />

1/m 4 b<br />

δΓ| 1/m i b = (Γ| 1/mi − Γ| 1/mi−1 )/Γparton<br />

<br />

<br />

≈ +0.29% δΓ<br />

1/m 3 b<br />

<br />

<br />

≈ −2.84% δΓ<br />

1/m 2 b<br />

≈ −4.29%<br />

Hence the impact on Vcb is only a small improvement due to the reduction of the uncertainty<br />

due to the higher-or<strong>de</strong>r terms of the HQE. However, once moments of differential distributions<br />

are consi<strong>de</strong>red, the impact of the higher-or<strong>de</strong>r terms becomes more pronounced, in particular<br />

for higher moments.<br />

References<br />

1. D. Benson, I. I. Bigi, T. Mannel <strong>and</strong> N. Uraltsev, Nucl. Phys. B 665 (2003) 367 [arXiv:hepph/0302262].<br />

2. K. Melnikov, Phys. Lett. B 666 (2008) 336 [arXiv:0803.0951 [hep-ph]].<br />

3. M. Dowling, A. Pak <strong>and</strong> A. Czarnecki, Phys. Rev. D 78 (2008) 074029 [arXiv:0809.0491<br />

[hep-ph]].<br />

4. T. Becher, H. Boos, E. Lunghi, JHEP 0712, 062 (2007). [arXiv:0708.0855 [hep-ph]].<br />

5. T. Mannel, S. Turczyk, N. Uraltsev, JHEP 1011, 109 (2010). [arXiv:1009.4622 [hep-ph]].<br />

6. I. Bigi, T. Mannel, S. Turczyk <strong>and</strong> N. Uraltsev, JHEP 1004 (2010) 073 [arXiv:0911.3322<br />

[hep-ph]].<br />

7. I.I. Bigi, M. Shifman <strong>and</strong> N. Uraltsev, Ann. Rev. Nucl. Part. Sci. 47 (1997) 591.

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