Hadronic Interactions and Nuclear Physics
|
|
|
- Dayna Wood
- 5 years ago
- Views:
Transcription
1 Williamsburg,VA LATT2008 7/2008 p. 1/35 Hadronic Interactions and Nuclear Physics Silas Beane University of New Hampshire
2 Williamsburg,VA LATT2008 7/2008 p. 2/35 Outline Motivation Signal/Noise Estimates MM MM...M MB BB The Future
3 Lattice QCD : So What?? Williamsburg,VA LATT2008 7/2008 p. 3/35
4 Williamsburg,VA LATT2008 7/2008 p. 3/35 Lattice QCD : So What?? Particle and Nuclear physics perspectives...
5 The particle physics perspective Williamsburg,VA LATT2008 7/2008 p. 4/35
6 Williamsburg,VA LATT2008 7/2008 p. 4/35 The particle physics perspective QCD is Background for beyond-the-standard-model physics (f K /f π, f Ds, B K,...)
7 The nuclear physics perspective Williamsburg,VA LATT2008 7/2008 p. 5/35
8 Williamsburg,VA LATT2008 7/2008 p. 5/35 The nuclear physics perspective Intrinsically interesting QCD physics! (Y N, Kπ, h πnn, nnn,...)
9 Williamsburg,VA LATT2008 7/2008 p. 6/35 The nuclear physics perspective Intrinsically interesting QCD physics! (Y N, Kπ, h πnn, nnn,...)
10 Williamsburg,VA LATT2008 7/2008 p. 7/35 NEOS p Σ interactions K + π Atoms Dirac collaboration interesting physics m π a 3/ a 0 : χpt p 2 - a 0 : χpt p 4 - a 0 : χpt p 6 fit A fit B fit C fit D Roy-Steiner (1-σ) χpt p 4 (1-σ) χpt p m π a 1/2
11 Williamsburg,VA LATT2008 7/2008 p. 7/35 NEOS p Σ interactions K + π Atoms Dirac collaboration interesting physics m π a 3/ a 0 : χpt p 2 - a 0 : χpt p 4 - a 0 : χpt p 6 fit A fit B fit C fit D Roy-Steiner (1-σ) χpt p 4 (1-σ) χpt p m π a 1/2 NPDgamma Experiment h πnn 0 O N (t) O π (τ 2 )Ow I=1 (τ 1 )ŌN(0) 0
12 Williamsburg,VA LATT2008 7/2008 p. 8/35 Signal/Noise Estimates Lepage (1989) Signal/Noise Estimates
13 Williamsburg,VA LATT2008 7/2008 p. 8/35 Signal/Noise Estimates Lepage (1989) PIONS : noise signal σ(t) θ(t) Signal/Noise Estimates e nm π t q`a2 A 2 0 NA0 e nm πt 1 N
14 Williamsburg,VA LATT2008 7/2008 p. 8/35 Signal/Noise Estimates Lepage (1989) PIONS : noise signal σ(t) θ(t) Signal/Noise Estimates e nm π t q`a2 A 2 0 NA0 e nm πt 1 N Noise independent of t!
15 Williamsburg,VA LATT2008 7/2008 p. 8/35 Signal/Noise Estimates Lepage (1989) PIONS : noise signal σ(t) θ(t) Signal/Noise Estimates e nm π t q`a2 A 2 0 NA0 e nm πt 1 N Noise independent of t! BARYONS : noise signal σ(t) θ(t) 1 N e (m p 3 2 m π)t
16 Williamsburg,VA LATT2008 7/2008 p. 8/35 Signal/Noise Estimates Lepage (1989) PIONS : noise signal σ(t) θ(t) Signal/Noise Estimates e nm π t q`a2 A 2 0 NA0 e nm πt 1 N Noise independent of t! BARYONS : noise signal σ(t) θ(t) 1 N e (m p 3 2 m π)t Exponential growth of noise!
17 Williamsburg,VA LATT2008 7/2008 p. 9/35 np ( 1 S 0 ) NPLQCD MILC/2064f21b676m010m050 signal/noise (Courtesy of Bedaque,Walker-Loud arxiv: )
18 Williamsburg,VA LATT2008 7/2008 p. 10/35 signal/noise Currently the main obstacle to lattice QCD calculations of nucleon and nuclear quantities is the signal/noise problem. Nuclear physics requires exponentially more resources than meson physics.
19 Williamsburg,VA LATT2008 7/2008 p. 10/35 signal/noise Currently the main obstacle to lattice QCD calculations of nucleon and nuclear quantities is the signal/noise problem. Nuclear physics requires exponentially more resources than meson physics. Theoretical fixes? z z 0 z L z L Orbifold boundary conditions z z 0 z L Bedaque,Walker-Loud/ arxiv:
20 Williamsburg,VA LATT2008 7/2008 p. 11/35 ππ Universal band tree (1966), one loop (1983), two loops (1996) Prediction (χpt + dispersion theory, 2001) l 4 from low energy theorem for scalar radius (2001) NPLQCD (2005, 2007) l 3 and l 4 from MILC (2004, 2006) l 3 from Del Debbio et al. (2006) l 3 and l 4 from ETM (2007) l 3 and l 4 from RBC/UKQCD (2007) l 3 and l 4 from PACS-CS (preliminary) Universal band tree (1966), one loop (1983), two loops (1996) Prediction (χpt + dispersion theory, 2001) E865 Ke4 (2003) isospin corrected DIRAC (2005) NA48 K3π (2006) NA48 Ke4 (preliminary) isospin corrected a a a a 0 0 (Courtesy of H. Leutwyler arxiv: )
21 Williamsburg,VA LATT2008 7/2008 p. 12/35 Hybrid of staggered sea quarks (MILC) and domain-wall valence quarks (LHPC+NPLQCD) (2+1) dynamical flavors Coarse lattices chopped from 64 to 32 with sources displaced in time and space Config Set Dimensions m π # configs # sources 2064f21b676m007m MeV f21b676m010m MeV f21b679m020m MeV f21b681m030m MeV f21b709m0062m MeV b coarse MILC fm bfine MILC 0.09 fm L 2.5 fm
22 Williamsburg,VA LATT2008 7/2008 p. 13/35 ππ-method E 0 (2, L) = 4π a ππ m π L 3 { 1 ( aππ ) ( aππ ) 2 [ I + I 2 J ] ( aππ ) 3 [ ] } + I 3 + 3IJ K + 8π2 3 a ππ r π L π L π L m π L 6 ππ + O ( L 7) I = lim Λ j i Λ X j i 0 1 i 2 4πΛ j = , J = X i 4 = , K = X i 0 i i 6 =
23 Williamsburg,VA LATT2008 7/2008 p. 14/35 0 ππ-bottom line -0.1 m π a ππ I= MA χ - PT (One Loop) χ - PT (Tree Level) CP-PACS (2004) (n f = 2) E 865 (2003) NPLQCD (MILC fine) NPLQCD (MILC coarse) m π / f π Savage/PAR-Mon-6pm
24 Williamsburg,VA LATT2008 7/2008 p. 15/35 Status of ππ χ - PT (Tree Level) NPLQCD (2007) E 865 (2003) NPLQCD (2005) MILC (2006)* MILC (2004)* CGL (2001) m π a I=2 ππ χpt (Tree Level) NPLQCD (2007) ± E 865 (2003) ± ± ± NPLQCD (2005) ± ± ± MILC (2006)* ± MILC (2004)* ± CGL (2001) ± m π a π+π+
25 Williamsburg,VA LATT2008 7/2008 p. 16/35 ππ Theoretical Developments ππ in χ-pt for Wilson lattice actions Buchoff/ arxiv: Aoki et al./ arxiv: /ps-b Wavefunction method for ππ phase shift Sasaki,Ishizuka/ arxiv: MM interactions from multi-m interactions NPLQCD/ arxiv: /par-tue-2:30pm
26 Williamsburg,VA LATT2008 7/2008 p. 17/35 m K + a K+K χ-pt (Tree Level) MILC coarse (b /= 0) MILC fine (b /= 0) physical point extrapolated with MAχ-PT KK m K + / f K+ m K + a K + K + = ± NPLQCD/arXiv : PAR-Mon-6pm
27 Williamsburg,VA LATT2008 7/2008 p. 18/35 meson-meson scattering 0 π + π + (Ι=2) 0 K + K + (I=1) m π a π +π χ - PT (Tree Level) Experiment NPLQCD (MILC coarse) CP-PACS m K a K+K χ-pt (Tree Level) NPLQCD (MILC coarse) physical line m π / f π m K / f K Mysterious disappearance of higher-order effects!
28 Williamsburg,VA LATT2008 7/2008 p. 19/35 MM...M n pions in a finite volume Detmold et al./ arxiv: , /par-tue-2:30pm Tan/ arxiv: E 0 (n, L) = 4π a ππ m π L 3 0 n A 2 1 I + π L aππ aππ 3 h + π L 0 1 aππ π L n A 8π2 a 3 ππ 2 m π L 6 r ππ + 2 ˆI2 + (2n 5)J I 3 (2n 7)IJ `5n i 2 41n + 63 ) K n 3 1 A η 3(L) L 6 + O `L 7 η 3 (L) = η 3 (µ) + 64π a ππ 4 m π (3 3 4π) log(l µ) 96 a 4 ππ (2Q + R) m π π2 dim reg /w MS : Q = , R =
29 Williamsburg,VA LATT2008 7/2008 p. 20/35 Three-body force NPLQCD/arXiv: , body Force mπ f L ΠΗ m Π f Π
30 Williamsburg,VA LATT2008 7/2008 p. 21/35 Pion condensate Μ I 1 m Π m Π 291 MeV Μ I 1 m Π m Π 352 MeV pion condensate n 2.5 fm 3 Ρ I n 2.5 fm 3 Ρ I Μ I 1 m Π 0.4 m Π 491 MeV Μ I 1 m Π m Π 591 MeV n 2.5 fm 3 Ρ I n 2.5 fm 3 Ρ I χ PT : ρ I = 1 2 f2 πµ I 1 m4 π µ 4 I!
31 Williamsburg,VA LATT2008 7/2008 p. 21/35 Pion condensate Μ I 1 m Π m Π 291 MeV Μ I 1 m Π m Π 352 MeV pion condensate n 2.5 fm 3 Ρ I n 2.5 fm 3 Ρ I Μ I 1 m Π 0.4 m Π 491 MeV Μ I 1 m Π m Π 591 MeV n 2.5 fm 3 Ρ I n 2.5 fm 3 Ρ I χ PT : ρ I = 1 2 f2 πµ I 1 m4 π µ 4 I! Three-body force is important!
32 Williamsburg,VA LATT2008 7/2008 p. 22/35 Μ K 1 m K Kaon condensate m Π 291 MeV m K 580 MeV NPLQCD/arXiv: Μ K 1 m K Kaon condensate m Π 352 MeV m K 597 MeV fm 3 Ρ K 2.5 fm 3 Ρ K Μ K 1 m K m Π 491 MeV m K 640 MeV Μ K 1 m K m Π 591 MeV m K 678 MeV fm 3 Ρ K 2.5 fm 3 Ρ K χ PT : ρ K = 1 2 f2 K µ K m4 K µ 3 K!
33 Williamsburg,VA LATT2008 7/2008 p. 22/35 Μ K 1 m K Kaon condensate m Π 291 MeV m K 580 MeV NPLQCD/arXiv: Μ K 1 m K Kaon condensate m Π 352 MeV m K 597 MeV fm 3 Ρ K 2.5 fm 3 Ρ K Μ K 1 m K m Π 491 MeV m K 640 MeV Μ K 1 m K m Π 591 MeV m K 678 MeV fm 3 Ρ K 2.5 fm 3 Ρ K χ PT : ρ K = 1 2 f2 K µ K m4 K µ 3 K! Why does χpt work so well??
34 Williamsburg,VA LATT2008 7/2008 p. 23/35 Meson-Baryon scattering Torok/PAR-Thu-8:50am Interesting phenomenology Important for baryon spectroscopy Juge/PAR-Tue-3:30pm
35 Williamsburg,VA LATT2008 7/2008 p. 23/35 Meson-Baryon scattering Torok/PAR-Thu-8:50am Interesting phenomenology Important for baryon spectroscopy Juge/PAR-Tue-3:30pm
36 Williamsburg,VA LATT2008 7/2008 p. 24/35 Baryon-Baryon scattering What should one calculate using lattice QCD? V NN (r) or δ NN (E)?
37 Williamsburg,VA LATT2008 7/2008 p. 24/35 Baryon-Baryon scattering What should one calculate using lattice QCD? V NN (r) or δ NN (E)? Historically nuclear physicists have used energy-independent potentials V NN (r) to fit NN phaseshifts with χ 2 /d.o.f. 1 over a wide range of (low) energies. V NN (r) = +
38 Williamsburg,VA LATT2008 7/2008 p. 24/35 Baryon-Baryon scattering What should one calculate using lattice QCD? V NN (r) or δ NN (E)? Historically nuclear physicists have used energy-independent potentials V NN (r) to fit NN phaseshifts with χ 2 /d.o.f. 1 over a wide range of (low) energies. V NN (r) = + = (χ 2 /d.o.f. 1)
39 V NN (k,k) [fm] Williamsburg,VA LATT2008 7/2008 p. 25/35 Baryon-Baryon scattering The modern viewpoint: Effective Field Theory S 0 Paris Bonn A Nijmegen I Nijmegen II Argonne v 18 CD Bonn Idaho A S 1 k [fm -1 ] (Courtesy of A. Schwenk et al. nucl-th/ )
40 V low k (k,k) [fm] Williamsburg,VA LATT2008 7/2008 p. 26/35 Use RG to integrate out Baryon-Baryon scattering = 4.1 fm -1 = 3.1 fm = 2.6 fm -1 = 2.1 fm k [fm -1 ] Argonne v 18 Paris CD Bonn Bonn A Idaho A Nijmegen I Nijmegen II
41 V low k (k,k) [fm] Williamsburg,VA LATT2008 7/2008 p. 26/35 Use RG to integrate out Baryon-Baryon scattering = 4.1 fm -1 = 3.1 fm = 2.6 fm -1 = 2.1 fm k [fm -1 ] Argonne v 18 Paris CD Bonn Bonn A Idaho A Nijmegen I Nijmegen II Bottom line: short distance part of V NN (r) not meaningful!
42 Williamsburg,VA LATT2008 7/2008 p. 27/35 Baryon-Baryon scattering Can one define and calculate V LATT BB (r)?
43 Williamsburg,VA LATT2008 7/2008 p. 27/35 Baryon-Baryon scattering Can one define and calculate V LATT BB (r)? NN: Aoki et al./ arxiv: /par-wed-3:50pm YN: Nemura et al./ arxiv: /par-wed-4:10pm Bethe-Salpeter wave function V LATT BB
44 Williamsburg,VA LATT2008 7/2008 p. 28/35 QQCD potentials V C (r) [MeV] np ( 1 S 0 ) pξ 0 ( 1 S 0 ) r [fm] m π =380MeV m π =529MeV m π =731MeV V (MeV) m π 368MeV m π 511MeV OPEP(α=0.36) r (fm) 1S Wilson quark action β = 5.7 b 0.137fm L 4.4fm
45 Williamsburg,VA LATT2008 7/2008 p. 29/35 PROBLEMS Detmold et al./ arxiv:hep-lat/ v1 Baryon-Baryon scattering
46 Williamsburg,VA LATT2008 7/2008 p. 29/35 PROBLEMS Detmold et al./ arxiv:hep-lat/ v1 Baryon-Baryon scattering V LAT T BB (r, E) Aoki/PAR-Wed-2:50pm
47 Williamsburg,VA LATT2008 7/2008 p. 29/35 PROBLEMS Detmold et al./ arxiv:hep-lat/ v1 Baryon-Baryon scattering V LAT T BB (r, E) Aoki/PAR-Wed-2:50pm V LAT T BB (r, E) δ LAT T BB (E)
48 Williamsburg,VA LATT2008 7/2008 p. 29/35 PROBLEMS Detmold et al./ arxiv:hep-lat/ v1 Baryon-Baryon scattering V LAT T BB (r, E) Aoki/PAR-Wed-2:50pm V LAT T BB (r, E) δ LAT T BB (E) V LAT T BB (r, E) δ LAT T BB (E )!!
49 Williamsburg,VA LATT2008 7/2008 p. 29/35 PROBLEMS Detmold et al./ arxiv:hep-lat/ v1 Baryon-Baryon scattering V LAT T BB (r, E) Aoki/PAR-Wed-2:50pm V LAT T BB (r, E) δ LAT T BB (E) V LAT T BB (r, E) δ LAT T BB (E )!! V LAT T BB (r, E, J) Aoki et al./in preparation V LAT T BB (r, E, J) r m 1 π V LAT T BB (r, E)??
50 Williamsburg,VA LATT2008 7/2008 p. 29/35 PROBLEMS Detmold et al./ arxiv:hep-lat/ v1 Baryon-Baryon scattering V LAT T BB (r, E) Aoki/PAR-Wed-2:50pm V LAT T BB (r, E) δ LAT T BB (E) V LAT T BB (r, E) δ LAT T BB (E )!! V LAT T BB (r, E, J) Aoki et al./in preparation V LAT T BB (r, E, J) r m 1 π V LAT T BB (r, E)?? QQCD : V LAT T NN (r) `M 0 α Φ m 2 π e m π r Dominates over Yukawa force!!
51 Williamsburg,VA LATT2008 7/2008 p. 30/35 Results: NN NN (singlet) a ( 1 S 0 ) [fm] NPLQCD (2006) (n f = 2+1) Aoki et al (2008) (n f = 0) Fukugita et al (1995) (n f = 0) m π [MeV]
52 Williamsburg,VA LATT2008 7/2008 p. 30/35 Results: NN NN (singlet) a ( 1 S 0 ) [fm] NPLQCD (2006) (n f = 2+1) Aoki et al (2008) (n f = 0) Fukugita et al (1995) (n f = 0) m π [MeV]
53 Williamsburg,VA LATT2008 7/2008 p. 31/35 Results: NN NN (triplet) a ( 3 S 1 ) [fm] NPLQCD (2006) (n f = 2+1) Aoki et al (2008) (n f = 0) Fukugita et al (1995) (n f = 0) m π [MeV]
54 Williamsburg,VA LATT2008 7/2008 p. 31/35 Results: NN NN (triplet) a ( 3 S 1 ) [fm] NPLQCD (2006) (n f = 2+1) Aoki et al (2008) (n f = 0) Fukugita et al (1995) (n f = 0) m π [MeV]
55 Williamsburg,VA LATT2008 7/2008 p. 32/35 Results: YN pξ 0 (QQCD) S 0 S a0 (fm) m π =0.135 GeV m π 2 (GeV 2 ) Nemura et al./ arxiv: /par-wed-4:10pm
56 Williamsburg,VA LATT2008 7/2008 p. 33/35 δ( k = 255 MeV ) (degrees) δ( k = 179 MeV ) (degrees) nλ ( 1 S 0 ) EFT 06 Juelich 04 Nijmegen NSC97f NPLQCD (2006) (n f = 2+1) m π (MeV) nσ ( 1 S 0 ) EFT 06 Juelich 04 Nijmegen NSC97f NPLQCD (2006) (n f = 2+1) m π (MeV) δ( k = 168 MeV ) (degrees) δ( k = 261 MeV ) (degrees) nλ ( 3 S 1 ) EFT 06 Juelich 04 Nijmegen NSC97f Results: YN NPLQCD (2006) (n f = 2+1) m π (MeV) nσ ( 3 S 1 ) EFT 06 Juelich 04 Nijmegen NSC97f NPLQCD (2006) (n f = 2+1) m π (MeV)
57 Williamsburg,VA LATT2008 7/2008 p. 34/35 The Future NN ( 3 S 1 ) b 0.125fm L 5fm 0.2 Tflop-years 2 Tflop-years 20 Tflop-years 4 a [fm] pion mass [MeV]
58 Williamsburg,VA LATT2008 7/2008 p. 35/35 Currently the main obstacle to lattice QCD calculations of nucleon and nuclear quantities is the signal/noise problem. Conclusion Nuclear physics requires exponentially more resources than meson physics. The advent of petascale computing will overcome this obstacle and allow the calculation of nuclear properties and interactions! The future is bright!
Meson Baryon Scattering
Meson Baryon Scattering Aaron Torok Department of Physics, Indiana University May 31, 2010 Meson Baryon Scattering in Lattice QCD Calculation of the π + Σ +, and π + Ξ 0 scattering lengths Aaron Torok
Isospin and Electromagnetism
Extreme Scale Computing Workshop, December 9 11, 2008 p. 1/11 Isospin and Electromagnetism Steven Gottlieb Extreme Scale Computing Workshop, December 9 11, 2008 p. 2/11 Questions In the exascale era, for
Light hadrons in 2+1 flavor lattice QCD
Light hadrons..., Lattice seminar, KITP, Jan 26, 2005. U.M. Heller p. 1/42 Light hadrons in 2+1 flavor lattice QCD Urs M. Heller American Physical Society & BNL Modern Challenges for Lattice Field Theory
Status of scalar quark matrix elements from Lattice QCD. André Walker-Loud
Status of scalar quark matrix elements from Lattice QCD André Walker-Loud Outline Nucleon matrix element calculations Direct method - 3 point function Indirect method - Feynman-Hellman Theorem Scalar Matrix
Nuclear Forces from Lattice QCD
Nuclear forces and their impact on structure, reactions and astrophysics TALENT 13 Lecture on Nuclear Forces from Lattice QCD Zohreh Davoudi University of Washington S-wave Luescher formula - a demonstration
EFT as the bridge between Lattice QCD and Nuclear Physics
EFT as the bridge between Lattice QCD and Nuclear Physics David B. Kaplan QCHSVII Ponta Delgada, Açores, September 2006 National Institute for Nuclear Theory Nuclear physics from lattice QCD? Not yet,
Baryon-Baryon Forces from Lattice QCD
Baryon-Baryon Forces from Lattice QCD quarks nuclei 1 fm neutron stars Tetsuo Hatsuda (Univ. Tokyo) T(r)opical QCD WS @ Cairns, Oct.1, 2010 [1] Why 10 fmbb forces? [2] NN force from lattice QCD [3] YN,
Lattice QCD studies of strangeness S = -2 baryon-baryon interactions
Lattice QCD studies of strangeness S = -2 baryon-baryon interactions Kenji Sasaki (University of Tsukuba) for HAL QCD collaboration HAL (Hadrons to Atomic nuclei from Lattice) QCD Collaboration S. Aoki
Lattice QCD From Nucleon Mass to Nuclear Mass
At the heart of most visible m Lattice QCD From Nucleon Mass to Nuclear Mass Martin J Savage The Proton Mass: At the Heart of Most Visible Matter, Temple University, Philadelphia, March 28-29 (2016) 1
Restless pions,, nuclear forces and statistical noise in lattice QCD. Paulo Bedaque U. of Maryland, College Park
Restless pions,, nuclear forces and statistical noise in lattice QCD Paulo Bedaque U. of Maryland, College Park What do we know? 1) NN phase shifts 1 S 0 neutron-proton What do we know? 2) Several potentials
The Gell-Mann Okubo Mass Relation among Baryons from Fully-Dynamical, Mixed-Action Lattice QCD
NT@UW-06-08 JLAB-xxxx UNH-06-02 The Gell-Mann Okubo Mass Relation among Baryons from Fully-Dynamical, Mixed-Action Lattice QCD Silas R. Beane, 1, 2 Kostas Orginos, 3, 2 and Martin J. Savage 4 (NPLQCD Collaboration)
arxiv: v1 [hep-lat] 3 Nov 2009
![arxiv: v1 [hep-lat] 3 Nov 2009](/thumbs/73/68223781.jpg "arxiv: v1 [hep-lat] 3 Nov 2009")
SU(2 chiral fits to light pseudoscalar masses and decay constants arxiv:0911.0472v1 [hep-lat] 3 Nov 2009 The MILC Collaboration: A. Bazavov, W. Freeman and D. Toussaint Department of Physics, University
Lattice QCD and flavour physics
Lattice QCD and flavour physics Vittorio Lubicz Workshop on Indirect Searches for New Physics at the time of LHC 15/02/2010-26/03/2010 OUTLINE: The accuracy of LQCD in the flavour sector the past (the
The Gell-Mann Okubo Mass Relation among Baryons from Fully-Dynamical Mixed-Action Lattice QCD
NT@UW-06-08 JLAB-THY-06-484 UNH-06-02 arxiv:hep-lat/0604013v1 16 Apr 2006 The Gell-Mann Okubo Mass Relation among Baryons from Fully-Dynamical Mixed-Action Lattice QCD Silas R. Beane, 1,2 Kostas Orginos,
hybrids (mesons and baryons) JLab Advanced Study Institute
hybrids (mesons and baryons) 2000 2000 1500 1500 1000 1000 500 500 0 0 71 the resonance spectrum of QCD or, where are you hiding the scattering amplitudes? real QCD real QCD has very few stable particles
D and B Meson Semileptonic Decays from the Lattice. Lattice QCD Meets Experiment Workshop April 26-27, 2010 Fermilab
D and B Meson Semileptonic Decays from the Lattice Lattice QCD Meets Experiment Workshop April 26-27, 2010 Fermilab presented by : Junko Shigemitsu The Ohio State University 1 Meson Semileptonic Decays
Low-energy aspects of amplitude analysis: chiral perturbation theory and dispersion relations
Low-energy aspects of amplitude analysis: chiral perturbation theory and dispersion relations Bastian Kubis Helmholtz-Institut für Strahlen- und Kernphysik (Theorie) Bethe Center for Theoretical Physics
Light pseudoscalar masses and decay constants with a mixed action
Light pseudoscalar masses and decay constants with a mixed action Jack Laiho Washington University Christopher Aubin and Ruth Van de Water Lattice 2008 July 15, 2008 William + Mary, July 15, 2008 p.1/21
Quarkonium Results from Fermilab and NRQCD
Quarkonium Results from Fermilab and NRQCD Paul Mackenzie mackenzie@fnal.gov International Workshop on Heavy Quarkonium Fermilab Sept. 20-22 2003 Thanks Christine Davies (HPQCD), Jim Simone Recent progress
Nuclear Force from Lattice QCD. [1] Why nuclear force now? [2] NN force from lattice QCD [3] BB and BM forces from lattice QCD [4] Summary and Future
![Nuclear Force from Lattice QCD. [1] Why nuclear force now? [2] NN force from lattice QCD [3] BB and BM forces from lattice QCD [4] Summary and Future](/thumbs/72/67542509.jpg "Nuclear Force from Lattice QCD. [1] Why nuclear force now? [2] NN force from lattice QCD [3] BB and BM forces from lattice QCD [4] Summary and Future")
Nuclear Force from Lattice QCD [1] Why nuclear force now? [2] NN force from lattice QCD [3] BB and BM forces from lattice QCD [4] Summary and Future Tetsuo Hatsuda (Univ. Tokyo) NFQCD, Feb 17, 2010 The
Nuclear Physics from Lattice QCD: The Spectrum, Structure and Interactions of Hadrons
Nuclear Physics from Lattice QCD: The Spectrum, Structure and Interactions of Hadrons Lattice QCD Executive Committee R. Brower, (Boston U.) N. Christ (Columbia U.), M. Creutz (BNL), P. Mackenzie (Fermilab),
Evgeny Epelbaum. Forschungszentrum Jülich & Universität Bonn
Evgeny Epelbaum KHuK Jahrestagung, GSI, 25.10.2007 Evgeny Epelbaum Forschungszentrum Jülich & Universität Bonn Outline Motivation & Introduction Few nucleons in chiral EFT: where do we stand Work in progress:
The theory of nuclear forces: Is the never-ending ending story coming to an end? R. Machleidt University of Idaho
The theory of nuclear forces: Is the never-ending ending story coming to an end? University of Idaho What s left to say? Put the recent progress into a wider perspective. Fill in some missing details.
B-meson decay constants with domain-wall light quarks and nonperturbatively tuned relativistic b-quarks
B-meson decay constants with domain-wall light quarks and nonperturbatively tuned relativistic b-quarks RBC and UKQCD collaborations Oliver Witzel Center for Computational Science Lattice 2013, Mainz,
Nucleon excited states on the lattice
Nucleon excited states on the lattice C.B. Lang, Valentina Verduci Graz, 12.12.12 Overview Motivation: Investigate the nucleon spectrum studying the π N scattering. The approach: How do we extract excited
Hadronic physics from the lattice
Hadronic physics from the lattice Chris Michael c.michael@liv.ac.uk University of Liverpool Hadronic physics from the lattice p.1/24 Hadronic Structure - Introduction What are hadrons made of? Is a meson
Nuclear structure I: Introduction and nuclear interactions
Nuclear structure I: Introduction and nuclear interactions Stefano Gandolfi Los Alamos National Laboratory (LANL) National Nuclear Physics Summer School Massachusetts Institute of Technology (MIT) July
Hadron structure from lattice QCD
Hadron structure from lattice QCD Giannis Koutsou Computation-based Science and Technology Research Centre () The Cyprus Institute EINN2015, 5th Nov. 2015, Pafos Outline Short introduction to lattice calculations
Nuclear Forces - Lecture 1 -
Physics Department, Tohoku University, June 30 July 2, 2014 Nuclear Forces - Lecture 1 - Historical Perspective R. Machleidt University of Idaho 1 Nuclear Forces - Overview of all lectures - Lecture 1:
Chiral perturbation theory with physical-mass ensembles
Chiral perturbation theory with physical-mass ensembles Steve Sharpe University of Washington S. Sharpe, Future of ChPT for LQCD 5/19/16 @ TUM-IAS EFT workshop 1 /35 ChPT for LQCD: Does it have a future?
(Towards) Baryon Resonances from Lattice QCD
(Towards) Baryon Resonances from Lattice QCD Daniel Mohler Fermilab Theory Group Batavia, IL, USA Paphos, October 2013 Daniel Mohler (Fermilab) Baryon Resonances from Lattice QCD Paphos, October 2013 1
MILC results and the convergence of the chiral expansion
MILC results and the convergence of the chiral expansion MILC Collaboration + (for part) HPQCD, UKQCD Collaborations Benasque Center for Science, July 27, 2004 p.1 Collaborators MILC Collaboration: C.
arxiv:hep-lat/ v1 3 Apr 1999
CP-PACS results for light hadron spectrum in quenched and two-flavor full QCD Yoshinobu Kuramashi for the CP-PACS Collaboration Department of Physics, Washington University, St. Louis, Missouri 63130 We
Meson wave functions from the lattice. Wolfram Schroers
Meson wave functions from the lattice Wolfram Schroers QCDSF/UKQCD Collaboration V.M. Braun, M. Göckeler, R. Horsley, H. Perlt, D. Pleiter, P.E.L. Rakow, G. Schierholz, A. Schiller, W. Schroers, H. Stüben,
PoS(LATTICE 2013)500. Charmonium, D s and D s from overlap fermion on domain wall fermion configurations
Charmonium, D s and D s from overlap fermion on domain wall fermion configurations,, Y. Chen, A. Alexandru, S.J. Dong, T. Draper, M. Gong,, F.X. Lee, A. Li, 4 K.F. Liu, Z. Liu, M. Lujan, and N. Mathur
A meson-exchange model for π N scattering up to energies s. Shin Nan Yang National Taiwan University
A meson-exchange model for π N scattering up to energies s 2 GeV Shin Nan Yang National Taiwan University Collaborators: S. S. Kamalov (Dubna) Guan Yeu Chen (Taipei) 18th International Conference on Few-body
Lattice QCD. Steven Gottlieb, Indiana University. Fermilab Users Group Meeting June 1-2, 2011
Lattice QCD Steven Gottlieb, Indiana University Fermilab Users Group Meeting June 1-2, 2011 Caveats I will borrow (shamelessly). 3 Lattice field theory is very active so there is not enough time to review
Unquenched spectroscopy with dynamical up, down and strange quarks
Unquenched spectroscopy with dynamical up, down and strange quarks CP-PACS and JLQCD Collaborations Tomomi Ishikawa Center for Computational Sciences, Univ. of Tsukuba tomomi@ccs.tsukuba.ac.jp 4th ILFTN
Chiral Dynamics with Pions, Nucleons, and Deltas. Daniel Phillips Ohio University
Chiral Dynamics with Pions, Nucleons, and Deltas Daniel Phillips Ohio University Connecting lattice and laboratory EFT Picture credits: C. Davies, Jefferson Lab. What is an Effective Field Theory? M=f(p/Λ)
Hyperon-Nucleon Scattering
Hyperon-Nucleon Scattering In A Covariant Chiral Effective Field Theory Approach Kai-Wen Li In collaboration with Xiu-Lei Ren, Bing-Wei Long and Li-Sheng Geng @INPC, Adelaide September, 2016 School of
Lattice QCD Christine Davies University of Glasgow, HPQCD collaboration. Lepton-photon 2007 Daegu, Korea
Lattice QCD 2007 Christine Davies University of Glasgow, HPQCD collaboration Lepton-photon 2007 Daegu, Korea QCD is key part of SM but quark confinement tricky a Lattice QCD enables calcn of QCD effects
How far can you go? Surprises & pitfalls in three-flavour chiral extrapolations
How far can you go? Surprises & pitfalls in three-flavour chiral extrapolations Sébastien Descotes-Genon Laboratoire de Physique Théorique CNRS & Université Paris-Sud 11, 91405 Orsay, France July 31 2007
Lecture 9 Valence Quark Model of Hadrons
Lecture 9 Valence Quark Model of Hadrons Isospin symmetry SU(3) flavour symmetry Meson & Baryon states Hadronic wavefunctions Masses and magnetic moments Heavy quark states 1 Isospin Symmetry Strong interactions
Multi-Channel Systems in a Finite Volume
INT-12-2b Multi-Channel Systems in a Finite olume RaúL Briceño In collaboration with: Zohreh Davoudi (arxiv:1204.1110 Motivation: Scalar Sector The light scalar spectrum Its nature remains puzzling Pertinent
Cascades on the Lattice
Cascade Physics - Jlab 2005 Cascades on the Lattice Kostas Orginos College of William and Mary - JLab LHP Collaboration LHPC collaborators R. Edwards (Jlab) G. Fleming (Yale) P. Hagler (Vrije Universiteit)
Lattice Studies of Baryon Resonances
Lattice Studies of Baryon Resonances HADRON SPECTRUM COLLABORATION J. Bulava, J. Dudek, R. Edwards, E. Engelson, Justin Foley, Bálint Joó, J. Juge, A. Lichtl,H.- W Lin, N. Mathur, C. Morningstar, D. Richards,
PROTON DECAY MATRIX ELEMENTS FROM LATTICE QCD. Yasumichi Aoki RIKEN BNL Research Center. 9/23/09 LBV09 at Madison
PROTON DECAY MATRIX ELEMENTS FROM LATTICE QCD Yasumichi Aoki RIKEN BNL Research Center 9/23/09 LBV09 at Madison Plan low energy matrix elements for N PS,l GUT QCD relation what is exactly needed to calculate
Effective Field Theories for lattice QCD
Effective Field Theories for lattice QCD Stephen R. Sharpe University of Washington S. Sharpe, EFT for LQCD: Lecture 1 3/21/12 @ New horizons in lattice field theory, Natal, Brazil 1 Outline of Lectures
Bayesian Fitting in Effective Field Theory
Bayesian Fitting in Effective Field Theory Department of Physics Ohio State University February, 26 Collaborators: D. Phillips (Ohio U.), U. van Kolck (Arizona), R.G.E. Timmermans (Groningen, Nijmegen)
H-dibaryon in Holographic QCD. Kohei Matsumoto (M2, YITP) (in collaboration with Hideo Suganuma, Yuya Nakagawa)
H-dibaryon in Holographic QCD Kohei Matsumoto (M2, YITP) (in collaboration with Hideo Suganuma, Yuya Nakagawa) 1. Aug. 2016 1 Contents 1. Introduction 2. Chiral Soliton Model 3. Holographic QCD 4. Results
PHYS 6610: Graduate Nuclear and Particle Physics I, Spring Institute for Nuclear Studies The George Washington University.
PHYS 6610: Graduate Nuclear and Particle Physics I H. W. Grießhammer INS Institute for Nuclear Studies The George Washington University Institute for Nuclear Studies Spring 2018 III. Descriptions 3. Lattice
PoS(LAT2006)094. The decay constants f B + and f D + from three-flavor lattice QCD
The decay constants f B + and f D + from three-flavor lattice QCD C. Bernard a, C. DeTar b, M. Di Pierro c, A.X. El-Khadra d, R.T. Evans d, E. Freeland e, S. Gottlieb f, U.M. Heller g, J.E. Hetrick h,
hg: Chiral Structure of Few-Nucleon Systems
Chiral Structure of Few-Nucleon Systems H. W. Grießhammer Center for Nuclear Studies, The George Washington University, Washington DC, USA D. R. Phillips: Chiral Dynamics with πs, Ns and s Done. hg: Chiral
BARYON PROPERTIES IN MESON MEDIUMS FROM LATTICE QCD
BARYON PROPERTIES IN MESON MEDIUMS FROM LATTICE QCD Amy Nicholson University of Maryland in collaboration with W. Detmold (MIT) Lattice 2013, Mainz, Germany, Thursday, August 1, 2013 MANY MESON SYSTEMS
Lecture 2: two-body William Detmold
Lecture 2: two-body William Detmold Massachusetts Institute of Technology INT Lattice Summer School, Seattle, August 13 th -17 th, 212 Hadron Interactions and Many-body Physics Lecture content Two particles
The kaon B-parameter from unquenched mixed action lattice QCD
The kaon B-parameter from unquenched mixed action lattice QCD Christopher Aubin Department of Physics, Columbia University, New York, NY, USA Department of Physics, College of William and Mary, Williamsburg,
Axial-Current Matrix Elements in Light Nuclei from Lattice QCD. Department of Physics, University of Washington, Box , Seattle, WA 98195, USA.
Axial-Current Matrix Elements in Light Nuclei from Lattice QCD, Emmanuel Chang and Michael L. Wagman Institute for Nuclear Theory, Seattle, Washington 98195-155, USA. E-mail: mjs5@uw.edu Silas R. Beane
Cold QCD. Meeting on Computational Nuclear Physics. Washington, DC July Thomas Luu Lawrence Livermore National Laboratory
Cold QCD Meeting on Computational Nuclear Physics Washington, DC July 2012 Thomas Luu Lawrence Livermore National Laboratory This work was performed under the auspices of the U.S. Department of Energy
Nuclear forces and their impact on structure, reactions and astrophysics
Nuclear forces and their impact on structure, reactions and astrophysics Lectures for Week 2 Dick Furnstahl Ohio State University July, 213 M. Chiral EFT 1 (as); χ-symmetry in NN scattering, QCD 2 (rjf)
NUCLEAR PHYSICS FROM LATTICE QCD
Twelfth Workshop on Non-Perturbative QCD Paris, June 10-14, 2013 NUCLEAR PHYSICS FROM LATTICE QCD Kostas Orginos QCD Hadron structure and spectrum Hadronic Interactions Nuclear physics Figure by W. Nazarewicz
Nuclear Forces - Lecture 1 - R. Machleidt University of Idaho
CNS Summer School, Univ. of Tokyo, at Wako campus of RIKEN, Aug. 18-23, 2005 Nuclear Forces - Lecture 1 - R. Machleidt University of Idaho 1 Nuclear Forces - Overview of all lectures - Lecture 1: History,
Lattice QCD investigation of heavy-light four-quark systems
Lattice QCD investigation of heavy-light four-quark systems Antje Peters peters@th.physik.uni-frankfurt.de Goethe-Universität Frankfurt am Main in collaboration with Pedro Bicudo, Krzysztof Cichy, Luka
Hyperonic lattice QCD potentials and hypernuclear few-body problems
Hyperonic lattice QCD potentials and hypernuclear few-body problems H. Nemura, for HAL QCD Collaboration S. Aoki2, T. Doi3, F. Etminan, S. Gongyo2, T. Hatsuda3, Y. Ikeda3, T. Inoue4, T. Iritani2, N. Ishii5,
arxiv: v1 [hep-lat] 30 Oct 2018
![arxiv: v1 [hep-lat] 30 Oct 2018](/thumbs/89/100543205.jpg "arxiv: v1 [hep-lat] 30 Oct 2018")
E-mail: genwang27@uky.edu arxiv:1810.12824v1 [hep-lat] 30 Oct 2018 Jian Liang E-mail: jian.liang@uky.edu Terrence Draper E-mail: draper@pa.uky.edu Keh-Fei Liu E-mail: liu@pa.uky.edu Yi-Bo Yang Institute
Is the up-quark massless? Hartmut Wittig DESY
Is the up-quark massless? Hartmut Wittig DESY Wuppertal, 5 November 2001 Quark mass ratios in Chiral Perturbation Theory Leutwyler s ellipse: ( mu m d ) 2 + 1 Q 2 ( ms m d ) 2 = 1 25 m s m d 38 R 44 0
Chiral Extrapolation of the Nucleon-Nucleon S-wave scattering lengths
Chiral Extrapolation of the Nucleon-Nucleon S-wave scattering lengths Jaume Tarrús Castellà Departament d Estructura i Constituents de la Matèria and Institut de Ciències del Cosmos Universitat de Barcelona
Renormalization group methods in nuclear few- and many-body problems
Renormalization group methods in nuclear few- and many-body problems Lecture 2 S.K. Bogner (NSCL/MSU) 2011 National Nuclear Physics Summer School University of North Carolina at Chapel Hill Lecture 2 outline
High Precision. Charm Physics. HISQ quarks
f % f K High Precision m Charm Physics $ with m N m Ds m D m D * HISQ quarks - m s D s m " - m #c "(1P-1S) 2m Bs,av -m! Christine m Davies Bc E. Follana, G. P. Lepage, R. Horgan, K. Hornbostel, C. McNeile,
arxiv: v1 [hep-lat] 24 Dec 2008
![arxiv: v1 [hep-lat] 24 Dec 2008](/thumbs/72/67235050.jpg "arxiv: v1 [hep-lat] 24 Dec 2008")
of hadrons from improved staggered quarks in full QCD arxiv:081.4486v1 [hep-lat] 4 Dec 008, a A. Bazavov, b C. Bernard, c C. DeTar, d W. Freeman, b Steven Gottlieb, a U.M. Heller, e J.E. Hetrick, f J.
PION PHYSICS FROM LATTICE QCD
MENU 2007 11th International Conference on Meson-Nucleon Physics and the Structure of the Nucleon September10-14, 2007 IKP, Forschungzentrum Jülich, Germany PION PHYSICS FROM LATTICE QCD Jie Hu,1, Fu-Jiun
Baryon semi-leptonic decay from lattice QCD with domain wall fermions
4th ILFTN Workshop at Hayama, Mar. 8-11, 2006 Baryon semi-leptonic decay from lattice QCD with domain wall fermions Shoichi Sasaki (RBRC/U. of Tokyo) in collabration with Takeshi Yamazaki (RBRC) Baryon
The Λ(1405) is an anti-kaon nucleon molecule. Jonathan Hall, Waseem Kamleh, Derek Leinweber, Ben Menadue, Ben Owen, Tony Thomas, Ross Young
The Λ(1405) is an anti-kaon nucleon molecule Jonathan Hall, Waseem Kamleh, Derek Leinweber, Ben Menadue, Ben Owen, Tony Thomas, Ross Young The Λ(1405) The Λ(1405) is the lowest-lying odd-parity state of
PoS(EPS-HEP2011)179. Lattice Flavour Physics
Rome University Tor Vergata" and INFN sez. Rome Tor Vergata" E-mail: nazario.tantalo@roma.infn.it I briefly discuss recent lattice calculations of a selected list of hadronic matrix elements that play
The light hadron spectrum from lattice QCD
Ch. Hoelbling with S. Durr Z. Fodor J. Frison S. Katz S. Krieg T. Kurth L. Lellouch Th. Lippert K. Szabo G. Vulvert The Budapest-Marseille-Wuppertal collaboration Rab 2008 Outline 1 Motivation 2 Setup
Nuclear Force from Lattice QCD
Department of Physics, University of Tokyo, Tokyo 113 0033, JAPAN E-mail: ishii@rarfaxp.riken.jp Sinya AOKI Graduate School of Pure and Applied Science, University of Tsukuba, Tukuba 305 8571, Ibaraki,
CHARMED BOTTOM BARYON SPECTROSCOPY. Zachary S. Brown, William Detmold, Stefan Meinel, Konstantinos Orginos
CHARMED BOTTOM BARYON SPECTROSCOPY Zachary S. Brown, William Detmold, Stefan Meinel, Konstantinos Orginos 1 OUTLINE Landscape of heavy baryon spectroscopy Details of our calculation Extrapolations Results
Few Body Methods in Nuclear Physics - Lecture I
Few Body Methods in Nuclear Physics - Lecture I Nir Barnea The Hebrew University, Jerusalem, Israel Sept. 2010 Course Outline 1 Introduction - Few-Body Nuclear Physics 2 Gaussian Expansion - The Stochastic
Towards Exploring Parity Violation with Lattice QCD. Towards Exploring Parity Violation with Lattice QCD. Brian Tiburzi 30 July 2014 RIKEN BNL
Towards Exploring Parity Violation with Lattice QCD Brian Tiburzi 30 July 2014 RIKEN BNL Research Center Towards Exploring Parity Violation with Lattice QCD Towards Exploring Parity Violation with Lattice
Future Directions for Nuclear Theory INT
Future Directions for Nuclear Theory INT David Kaplan - DNP Meeting - October 11, 2007 What are some of the big advances in physics of recent years? INT David Kaplan - QCD Town Meeting - January 12-14,
The nucleon mass and pion-nucleon sigma term from a chiral analysis of lattice QCD world data
The nucleon mass and pion-nucleon sigma term from a chiral analysis of lattice QCD world data L. Alvarez-Ruso 1, T. Ledwig 1, J. Martin-Camalich, M. J. Vicente-Vacas 1 1 Departamento de Física Teórica
Quantum ChromoDynamics and Hadron Physics. Anthony W. Thomas : CSSM Adelaide
Quantum ChromoDynamics and Hadron Physics Anthony W. Thomas : CSSM Adelaide Outline PART A : Hadron Structure Lattice QCD ) New insight into the QCD vacuum with and without quarks Precise calculations
National Nuclear Physics Summer School Lectures on Effective Field Theory. Brian Tiburzi. RIKEN BNL Research Center
2014 National Nuclear Physics Summer School Lectures on Effective Field Theory I. Removing heavy particles II. Removing large scales III. Describing Goldstone bosons IV. Interacting with Goldstone bosons
Lattice QCD and Nuclear Physics
Lattice Hadron Physics Newport News, July 3 - August 3 6 Lattice QCD and Nuclear Physics Kostas Orginos The College of William and Mary JLab NPLQCD collaborators S Beane (UNH) P Bedaque (LBNL) E Pallante
Overview of Jefferson Lab Physics Program. David Richards 1 st June, 2008 HUGS
Overview of Jefferson Lab Physics Program David Richards 1 st June, 2008 HUGS Why are we here? Describe how the fundamental building blocks of the nucleus, the protons and neutrons, are built from the
arxiv:nucl-th/ v1 28 Aug 2001
A meson exchange model for the Y N interaction J. Haidenbauer, W. Melnitchouk and J. Speth arxiv:nucl-th/1862 v1 28 Aug 1 Forschungszentrum Jülich, IKP, D-52425 Jülich, Germany Jefferson Lab, 1 Jefferson
arxiv: v1 [hep-lat] 7 Oct 2007
![arxiv: v1 [hep-lat] 7 Oct 2007](/thumbs/88/116044641.jpg "arxiv: v1 [hep-lat] 7 Oct 2007")
Charm and bottom heavy baryon mass spectrum from lattice QCD with 2+1 flavors arxiv:0710.1422v1 [hep-lat] 7 Oct 2007 and Steven Gottlieb Department of Physics, Indiana University, Bloomington, Indiana
Transverse Momentum Distributions of Partons in the Nucleon
Lattice 2008, Williamsburg 2008-07-18 Transverse Momentum Distributions of Partons in the Nucleon Bernhard Musch Technische Universität München presenting work in collaboration with LHPC and Philipp Hägler
Double poles in Lattice QCD with mixed actions
San Francisco State University E-mail: maarten@stars.sfsu.edu Taku Izubuchi Kanazawa University and Brookhaven National Laboratory E-mail: izubuchi@quark.phy.bnl.gov Yigal Shamir Tel Aviv University E-mail:
Quark Physics from Lattice QCD
Quark Physics from Lattice QCD K. Szabo published in NIC Symposium 2018 K. Binder, M. Müller, A. Trautmann (Editors) Forschungszentrum Jülich GmbH, John von Neumann Institute for Computing (NIC), Schriften
Baryon spectroscopy with spatially improved quark sources
Baryon spectroscopy with spatially improved quark sources T. Burch,, D. Hierl, and A. Schäfer Institut für Theoretische Physik Universität Regensburg D-93040 Regensburg, Germany. E-mail: christian.hagen@physik.uni-regensburg.de
The electric dipole moment of the nucleon from lattice QCD with imaginary vacuum angle theta
The electric dipole moment of the nucleon from lattice QCD with imaginary vacuum angle theta Yoshifumi Nakamura(NIC/DESY) for the theta collaboration S. Aoki(RBRC/Tsukuba), R. Horsley(Edinburgh), YN, D.
QCD thermodynamics with two-flavours of Wilson fermions on large lattices
QCD thermodynamics with two-flavours of Wilson fermions on large lattices Bastian Brandt Institute for nuclear physics In collaboration with A. Francis, H.B. Meyer, O. Philipsen (Frankfurt) and H. Wittig
Λ(1405) and Negative-Parity Baryons in Lattice QCD. Y.Nemoto (RIKEN-BNL) N.Nakajima (Kochi U.) H.Matsufuru (KEK) H.Suganuma (Tokyo Inst.Tech.
Λ(1405) and Negative-Parity Baryons in Lattice QCD Y.Nemoto (RIKEN-BNL) N.Nakajima (Kochi U.) H.Matsufuru (KEK) H.Suganuma (Tokyo Inst.Tech.) The Λ(1405) Particle Mass: ~1406.5 MeV Width: ~50 MeV I=0,
Towards thermodynamics from lattice QCD with dynamical charm Project A4
Towards thermodynamics from lattice QCD with dynamical charm Project A4 Florian Burger Humboldt University Berlin for the tmft Collaboration: E.-M. Ilgenfritz (JINR Dubna), M. Müller-Preussker (HU Berlin),
Symposium in honor of Keh-Fei Liu on the occasion of his 60th Birthday
Symposium in honor of Keh-Fei Liu on the occasion of his 60th Birthday A good physicist wide knowledge, deep intuition, full of innovative ideas, up-todate in theory and experiment Visionary For example:
Pseudoscalar Flavor-Singlet Physics with Staggered Fermions
Pseudoscalar Flavor-Singlet Physics with Staggered Fermions UKQCD Collaboration, Alan Irving, Chris M. Richards Department of Mathematical Sciences, University of Liverpool, Liverpool, L69-7ZL, UK E-mail:
Bound states on the lattice
Bound states on the lattice Daniel Mohler Admont, February, 2017 Daniel Mohler (HIM) Bound states on the lattice Admont, February, 2017 1 / 55 A simplistic take on fermion discretizations family staggered
Chiral extrapolation of lattice QCD results
Chiral extrapolation of lattice QCD results Ross Young CSSM, University of Adelaide MENU 2010, May 31 June 4 2010 College of William & Mary Williamsburg, VA, USA Nucleon couples strongly to pions in QCD
RG scaling at chiral phase transition in two-flavor QCD
RG scaling at chiral phase transition in two-flavor QCD Graduate School of Science, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-826, Japan E-mail: ishikawa@theo.phys.sci.hiroshima-u.ac.jp Yoichi
The Λ(1405) is an anti-kaon nucleon molecule. Jonathan Hall, Waseem Kamleh, Derek Leinweber, Ben Menadue, Ben Owen, Tony Thomas, Ross Young
The Λ(1405) is an anti-kaon nucleon molecule Jonathan Hall, Waseem Kamleh, Derek Leinweber, Ben Menadue, Ben Owen, Tony Thomas, Ross Young The Λ(1405) The Λ(1405) is the lowest-lying odd-parity state of