k - d 原子 の理論計算の現状と 今後の課題
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K - d 原子 の理論計算の現状と 今後の課題. Shota Ohnishi (Tokyo Inst. Tech. / RIKEN). in collaboration with Yoichi Ikeda (RIKEN) Tetsuo Hyodo (YITP, Kyoto Univ. ) Emiko Hiyama (RIKEN) Wolfram Weise (ECT*). K bar N interaction. Experimental data used to determine model parameters. - PowerPoint PPT PresentationTRANSCRIPT
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K-d原子の理論計算の現状と今後の課題Shota Ohnishi
(Tokyo Inst. Tech. / RIKEN)in collaboration with
Yoichi Ikeda (RIKEN)Tetsuo Hyodo (YITP, Kyoto Univ. )
Emiko Hiyama (RIKEN)Wolfram Weise (ECT*)
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KbarN interaction
K-p cross section: above KbarN threshold energy (w/ large error)
Branching ratio kaonic atom
L(1405) : below KbarN threshold energy (one pole or two pole <-> L(1405) or L(1420))
Experimental data used to determine model parameters
: at/just below KbarN threshold energy
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Energy dependence of KbarN interaction
WT LagrangianDerivative coupling E-dependent E-independent
Ikeda, Sato, PRC76, 035203(2007); Ikeda, Kamano, Sato, PTP124, 533(2010)
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Signature of the KbarNN resonance
E-dep.
Ohnishi, Ikeda, Kamano, Sato arXiv:1302.2301[nucl-th]
Significant difference on production spectracan be used to obtain KbarN interaction information
E-indep.
to appear in PRC
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Kaonic hydrogenCoulomb
0-8.6keV
Only Coulomb Coulomb + strong int.
1s
L(1405)
1s kaonic hydrogen
Improved Deser formula
Important constraint on K-p scattering length from the energy shift and width
Meissner, Raha, Rusetsky, Eur. Phys. J. C41 (2005) 213.
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Kaonic hydrogenSIDDHARTA Collaboration Phys. Lett. B 704 (2011) 113.
SIDDHARTA measurement of the energy shift and width of the 1s state :
Improved Deser formula
Ikeda, Hyodo, Weise Nucl. Phys. A 881 (2012) 98.2013/8/5 6
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Kaonic deuterium
K-p and K-d scattering lengths scattering lengths in I=0 and I=1 channels
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Deser formulaK--nuclear optical potential of the tr form :
neglect finite size effects
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Importance of multiple scattering• large cancelation of impulse approx. does NOT work• strong charge exchange interaction
between and worse convergence of scattering series
Impulse approx. Double scattering
+
+ …
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Rusetsky formulaimpulse approximation
double scattering
Rusetsky formula (all orders of the multiple scattering)
daK-d : three-body LECs neglect2013/8/5 10
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Improved Deser formulaimproved Deser formula
Coulomb correction
QED relativistic correction necessary
electronic vacuum polarization is amplified by powers of
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full optical potential
Here, multiple scattering, NN-pair correlations, finite nuclear size effect and so on are taken into account except for deuteron excitations.
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Uehling potentialFor kaonic atom, electron vacuum polarization effect is so large, that if we try to solve Schrödinger equation for K-pn three-body system to study deuteron excitations effect, we also need to consider about correction of Coulomb force.
for non-relativistic limit
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modification of Coulomb potential
• As a first step to study K-d atom,– K-p atom
Deser formula
imp. Deser formula
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K-p interaction• We employ the Gaussian local potential based on chiral
effective field theory
Parameters are fitted to reproduce the amplitude of Ikeda, Hyodo, Weise Nucl. Phys. A 881 (2012) 98.
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We study the 1s energy shift by solving the Schrodinger equation with only Coulomb potential and with Coulomb and strong interaction using the variational method.
We obtain the value between Deser formula and improved Deser formula.
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electron vacuum polarization
Coulomb vs Coulomb + strong -> Coulomb + Uehling vs Coulomb + Uehling + strong
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Future work• How to handle the effect of electron vacuum polarization
effect.– Lamb shift, K-d
• Three-body caluculation of the K-pn• Faddeev calculation of AK-d
Summary• Deser formula and improved Deser formula– Effect of electron vacuum polarization
• K-p– Uehling potential
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