Study of bound and scattering states of few-body systems with the HH method
|
|
- Candace Knight
- 5 years ago
- Views:
Transcription
1 Study of bound and scattering states of few-body systems with the HH method M. Viviani INFN, Sezione di Pisa & Department of Physics, University of Pisa Pisa (Italy) Electron-Nucleus Scattering XIII, June 23-27, 214 Mini-symposium to honor Professor Sergio Rosati on his 8th Birthday M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 1 / 32
2 Outline 1 The rise (and fall...) of the Few-Body Pisa Group 2 3NF effects in few-nucleon systems p d scattering p 3 He scattering p 3 H scattering Collaborators S. Rosati, A. Kievsky & L.E. Marcucci - INFN & Pisa University, Pisa (Italy) L. Girlanda - INFN & Universitá del Salento, Lecce (Italy) R. Schiavilla, M. Piarulli, A. Baroni, F. Spadoni - Jefferson Lab. & ODU, Norfolk (VA, USA) S. Pastore - USC, Columbia (SC, USA) M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 2 / 32
3 The rise (and fall...) of the Few-Body Pisa Group The Jastrow period ( ) B. Barsella and S. Rosati, On the Effect of n-p Tensor Forces in 3 H Λ, Nuovo Cimento 2, 914 (1961). J. Murphy and S. Rosati, A two-body method for the bound states of a three-body system, Nucl. Phys. 63, 625 (1965). M. Barbi and S. Rosati, Direct numerical solution of the three-body problem, Phys. Rev. 147, 73 (1966). S. Fantoni, L. Panattoni, and S. Rosati, Calculation on nuclear 3-body and 4-body systems with jastrow-type correlated wave functions, Nuovo Cimento 69, 8 (197). L. Lovitch and S. Rosati, Bound State Solution of the Two-Nucleon Schroedinger Equation with Tensor Forces, Comp. Phys. Com. 2, 353 (1971). Ψ = g(r 12 )g(r 13 )g(r 23 ) δ Ψ H E Ψ = Euler equation: for an S-state and for a central spin-independent potential v(r): 1 ( ) M 2 g(r)+ v(r)+w[g, r] g(r) = Eg(r) Non-linear iterative solution M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 3 / 32
4 Interlude 1 The Many-body period ( ) [S. Fantoni and S. Rosati, Expansion Procedure for Jastrow-Type Correlated Wave Functions, Nuovo Cimento A 1, 145 (1972)] My first conference: Third International Conference on Recent Progress in Many-Body Theories Odenthal-Altemberg, Germany, August 29 September 3, 1983 A wonderful 2-days trip from Pisa to Altenberg (and back) with Sergio, Stefano, and Adelchi, crammed in Stefano s FIAT 127 M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 4 / 32
5 A new start... Improvements of the wave functions and extension to realistic potentials ( ) From the CHO to the CHH expansion (selected papers) A. Kievsky, S. Rosati and M. Viviani, Euler and Correlated Harmonic Oscillator Wave Functions for Three-Nucleon Systems, Nucl. Phys. A 51, 53 (1989). Few-Body Systems 9, 1 (199). M. Viviani, A. Kievsky and S. Rosati, Correlated Hyperspherical Harmonic Calculations for Three- and Four-Body Systems, Nuovo Cimento A 15, 1473 (1992). A. Kievsky, M. Viviani and S. Rosati, The Three-Nucleon Bound-State with Realistic Soft and Hard Core Potentials, Nucl. Phys. A 551, 241 (1993). A. Kievsky, M. Viviani and S. Rosati, Variational Calculations for Scattering States in Three-Nucleon Systems, Few-Body Sys. Suppl. 7, 278 (1994). M. Viviani, A. Kievsky and S. Rosati, Calculation of the Alpha-Particle Ground-State, Few-Body Systems 18, 25 (1995). A. Kievsky, L. E. Marcucci, S. Rosati and M. Viviani, High-Precision Calculation of the Triton Ground State within the Hyperspherical Harmonics Method, Few-Body Systems 22, 1 (1997). M. Viviani, S. Rosati and A. Kievsky, Neutron- 3 H and Proton- 3 He Zero Energy Scattering, Phys. Rev. Lett. 81, 158 (1998). M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 5 / 32
6 The goal: reach the accuracy achieved by other groups (Friar and Coll., Glöckle and Coll., Kamimura and Coll.,...) + be able to treat realistic interactions, also hard-core potentials full inclusion of the Coulomb interaction A y puzzle in p d elastic scattering Ψ = N c i=1,3α=1 { [ ] } ] f α(r jk )g(r ij )g(r ik ) Y (ˆx lα i)y (ŷ Lα i) [(s j s k ) Sα s i [(t j t k ) Tα t i F α(x i, y i ) ]Λα Σ α JJ T z α F α(x i, y i ) expanded first in either HO or HH basis CHH=correlated Hyperspherical harmonics expansion ( PHH if g = 1) Method B (MeV) T (MeV) P s (%) P D (%) P P (%) AV18 potential PHH Witala et al. (23) Hamada-Johnston (hard-core) potential CHH Delves & Hennel (1971) M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 6 / 32
7 Interlude 2 The first Few-Body conference: 12th International Conference on Few-Body Problems in Physics (FBXII) Vancouver, B.C., Canada, July 2-8, 1989 M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 7 / 32
8 Many ideas... Some of the ideas produced by Sergio during the many discussions we had in those years... M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 8 / 32
9 One-point integration... Idea: to integrate one needs to compute the integrand in just one point b I = dx f(x) = (b a) f(x ) a It would be very useful in case of multidimensional integration x x I = dx 1... dx n f(x 1,...,x n) = Volume f( x 1,..., x n) Unfortunately we could not succeed... M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 9 / 32
10 The last period Extension of the method to non-local momentum space potentials (25 present) no correlation factor the interactions are softer & easy to trasform the wave function from coordinate to momentum space (and viceversa) (selected papers) M. Viviani, A. Kievsky and S. Rosati, Calculation of the Alpha Particle Ground State within the Hyperspherical Harmonic Basis, Phys. Rev. C 71, 246 (25) M. Viviani, L. E. Marcucci, S. Rosati, A. Kievsky and L. Girlanda, Variational Calculation on A=3 and 4 Nuclei with Non-Local Potentials, Few-Body Systems 39, 159 (26) A. Kievsky, S. Rosati, M. Viviani, L. E. Marcucci, L. Girlanda, A High-Precision Variational Approach to Three- and Four-Nucleon Bound and Zero-Energy Scattering States, J. Phys. G: Nucl. Part. Phys. 35, 6311 (28) M. Viviani, A. Deltuva, R. Lazauskas, J. Carbonell, A. C. Fonseca, A. Kievsky, L.E. Marcucci, and S. Rosati, Benchmark calculation of n- 3 H and p- 3 He scattering, PRC 84, 541 (211) M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 1 / 32
11 Interlude 3 18th International Conference on Few-Body Problems in Physics (FBXII) Santos, SP, Brazil, August 21-26, 26 M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 11 / 32
12 Applications EM and Weak transitions in light nuclei p, p d, and hep astrophysical factor Form factors of 3 H, 3 He, and 4 He Parity-violation Longitudinal polarization in n + 3 He p + 3 H Study of chiral effective field theory potentials and currents.5 S(E c.m. ) (ev b) LUNA Griffiths et al. Schmid et al E c.m. (kev) M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 12 / 32
13 3NF effects in few-nucleon systems Nuclear Dynamics: the EFT approach Chiral effective field theory (χeft): N π interaction dictated by chiral symmetry [Weinberg (199), Bernard, Kaiser, & Meissner (1995), Ordonéz, Ray, & van Kolck (1996), Epelbaum, Meissner, & Epelbaum (1998),...] Pionless effective field theory (π/eft): low energy processes [Kaplan, Savage, & Wise (1998), van Kolck (1999),...] Study of A = 3, 4 reactions using χeft Test of the derived NN & 3N interactions Different accurate theoretical techniques FY/AGS equations in momentum space [Witala et al., ], [Deltuva & Fonseca, 27, 212] FY equations in coordinate space [Lazauskas & Carbonell, 29, 212] HH expansion + Kohn variational principle NCSM/RG method [Navratil, Quaglioni & Coll., ] A y puzzle, energy production (NIF), reactions of astrophysical interest, study of fundamental symmetries, etc. muon capture on d MUSUN [Marcucci, 211 ],... M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 13 / 32
14 A y puzzle NN interaction Old models : Argonne V18, CD-Bonn, Nijmengen (χ 2 1) Derived from χeft J-N3LO [Epelbaum and Coll, ] N3LO5 & N3LO6 [Entem & Machleidt, 23 & 211] E cm =266 kev E cm = 431 kev E cm = 666 kev E p =2.25 MeV E p =4 MeV E p =5.54 MeV A y George Fisher N3LO5 AV18 Fisher Alley Alley A y E cm = 1.33 MeV E cm = 1.66 MeV E cm = 2. MeV θ cm θ cm θ cm A = 3 Delicate balance between 4 P j waves θ [c.m.] θ [c.m.] θ [c.m.] A = 4 Confirmed also for other NN potentials (Deltuva & Fonseca 27) dashed lines: N3LO5, dotted-dashed lines: N3LO5/UIX, solid lines N3LO5/N2LO5* M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 14 / 32
15 Inclusion of the 3NF Models from EFT Illinois models Fujita Miyazawa S wave scattering pion rings [Pieper et al., 21] 3π exchanges and π rings Illinois-7: coefficients chosen to reproduce the A = 4 12 spectrum 3n force at N 2 LO: 2 unknonw LEC s c d & c E + cutoff Λ [Epelbaum et al., 22] N2LO5 & N2LO6: LECs fixed by L. Marcucci (see next slide) N 3 LO & N 4 LO pion exchanges: [Krebs, Epelbaum, et al., ( )] 1 Contact terms at N 4 LO: [Girlanda, Kievsky, MV, (211)] (a) (b) (c) (d) (e) (f) M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 15 / 32
16 New fit of c D and c E Sensitivity to c D and c E c D enters also in β-decay processes [Gardestig & Phillips, 26], [Gazit et al., 29] d R = M c 4πf πg D + M A 3 (c 3 + 2c 4 )+ 1 6 d R (and thus c D ) can be fixed from the tritium Gamow-Teller m.e. GT EXPT =.955±.4 d R X cd Models under study: Model Λ [MeV] c D c E B( 4 He) [MeV] a 2 (n d) [fm] N3LO N3LO5/N2LO N3LO6/N2LO AV AV18/IL Expt ±.3±.7 Expt a 2 (n d): K. Schoen et al., 23 M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 16 / 32
17 HH expansion Example: p 3 He elastic scattering Ω ± LS (A, B) = 1 N N perm.=1 [Y L (ŷ p ) [φ A φ B ] S ] JJ z ( f L (y G L(η, q AB y p) p) ± i F ) L(η, q AB y p) q AB y p q AB y p Ψ LS = n,[k] a LS,[K] n,[k] + Ω LS (p, 3 He) L S S LS,L S Ω+ L S (p, 3 He) n,[k] HH states S LS,L S = S-matrix a LS,[K] and S LS,L S computed using the Kohn variational principle For a review, see [J. Phys. G: Nucl. Part. Phys. 35, 6311 (28) ] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 17 / 32
18 HH expansion Example: p 3 He elastic scattering Ω ± LS (A, B) = 1 N N perm.=1 [Y L (ŷ p) [φ A φ B ] S ] JJ z ( f L (y G L(η, q AB y p) p) ± i F ) L(η, q AB y p) q AB y p q AB y p Ψ LS = n,[k] a LS,[K] n,[k] + Ω LS (p, 3 He) L S S LS,L S Ω+ L S (p, 3 He) n,[k] HH states S LS,L S = S-matrix a LS,[K] and S LS,L S computed using the Kohn variational principle For a review, see [J. Phys. G: Nucl. Part. Phys. 35, 6311 (28) ] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 17 / 32
19 HH expansion Example: p 3 He elastic scattering Ω ± LS (A, B) = 1 N N perm.=1 [Y L (ŷ p) [φ A φ B ] S ] JJ z ( f L (y G L(η, q AB y p) p) ± i F ) L(η, q AB y p) q AB y p q AB y p Ψ LS = n,[k] a LS,[K] n,[k] + Ω LS (p, 3 He) L S S LS,L S Ω+ L S (p, 3 He) n,[k] HH states S LS,L S = S-matrix a LS,[K] and S LS,L S computed using the Kohn variational principle For a review, see [J. Phys. G: Nucl. Part. Phys. 35, 6311 (28) ] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 17 / 32
20 Convergence n 3 H at E cm = 3 MeV, 3 P 2 wave 1 δ(k)-δ(k-2).1.1 AV18 N3LO-Idaho K Convergence with the grand-angular quantum number M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 18 / 32
21 Benchmark test of 4N scattering calculations [PRC 84, 541 (211)] p 3 He elastic scattering dσ/dω [mb/sr] A y A y MeV Famularo 1954 Fisher 26 AGS 6 12,4,2 Fisher 26 George ,2,1 Daniels Mcdonald 1964 Fisher Fisher MeV 6 12 Daniels Alley MeV Mcdonald Alley 1993 Daniels N3LO5 potential AGS= Deltuva & Fonseca FY= Lazauskas & Carbonell M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 19 / 32
22 Benchmark test of 4N scattering calculations [PRC 84, 541 (211)] p 3 He elastic scattering dσ/dω [mb/sr] A y A y MeV Famularo 1954 Fisher 26 AGS HH 6 12,4,2 Fisher 26 George ,2,1 Daniels Mcdonald 1964 Fisher Fisher MeV 6 12 Daniels Alley MeV Mcdonald Alley 1993 Daniels N3LO5 potential AGS= Deltuva & Fonseca FY= Lazauskas & Carbonell M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 19 / 32
23 Benchmark test of 4N scattering calculations [PRC 84, 541 (211)] p 3 He elastic scattering dσ/dω [mb/sr] A y A y MeV Famularo 1954 Fisher 26 AGS HH FY 6 12,4,2 Fisher 26 George ,2,1 Daniels Mcdonald 1964 Fisher Fisher MeV 6 12 Daniels Alley MeV Mcdonald Alley 1993 Daniels N3LO5 potential AGS= Deltuva & Fonseca FY= Lazauskas & Carbonell M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 19 / 32
24 Effect of the N 2 LO & Illinois 3NF in p d scattering p-d scattering at E p =3 MeV A y.2 it NN only NN+3N AV18/IL θ θ Bands: results obtained for Λ = 5 & Λ = 6 MeV NN: N3LO5 & N3LO6 NN+3N: N3LO5/N2LO5 & N3LO6/N2LO6 M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 2 / 32
25 Study of the N 3 LO & N 4 LO 3NF in p d scattering [Krebs, Epelbaum, et al., 212,213] First study in n d scattering [Witala et al., 213].2 (a) (b) (c) (d) (e) (f) A y.1 E n =14.1 MeV d(n,n)d (1) (2) (3) (4) (5) (6) (7) (8) (9) (1) Θ cm (1) (2) (3) + many others diagrams... (4) green band: J-N3LO NN interaction only magenta band: + N 3 LO 3NF (no 2π contact terms) Very complicate implementation! M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 21 / 32
26 3N contact terms at N 4 LO (1) [Girlanda, Kievsky, MV, PRC 84, 141 (211)] Two of the operators O = spatial derivatives (N O 1 N)(N O 2 N)(N O 3 N) 146 possible combinations, which can be reduced to 1 using Fierz transformation and other constraints O 1 O 2 O [1,τ 1 τ 2,τ 1 τ 3 ] σ 1 2 σ 2 [1,τ 1 τ 2,τ 1 τ 3 ] σ 2 2 σ 1 [1,τ 1 τ 2,τ 1 τ 3 ] σ 1 σ 2 [1,τ 1 τ 2,τ 1 τ 3 ] σ 1 2 σ 3 [1,τ 1 τ 2,τ 1 τ 3,τ 2 τ 3 ] σ 3 2 σ 1 [1,τ 1 τ 2,τ 1 τ 3,τ 2 τ 3 ] σ 1 σ 3 [1,τ 1 τ 2,τ 1 τ 3,τ 2 τ 3 ] σ 1 [τ 1 τ 2 τ 3 ] σ 3 [τ 1 τ 2 τ 3 ] σ 1 σ 2 σ 3 [τ 1 τ 2 τ 3 ] σ 2 1 σ 1 σ 3 [τ 1 τ 2 τ 3 ] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 22 / 32
27 3N contact terms at N 4 LO (2) Final form of the new 3NF terms V = i j k [ ] (E 1 + E 2 τ i τ j + E 3 σ i σ j + E 4 τ i τ j σ i σ j ) Z ij)+2 Z (r ij) r ij Z (r ik ) [ +(E 5 + E 6 τ i τ j )S ij Z ij) Z (r ] ij) Z (r ik ) r ij +(E 7 + E 8 τ i τ k )(L S) ij Z (r ij) r ij Z (r ik ) +(E 9 + E 1 τ j τ k )σ j ˆr ij σ k ˆr ik Z (r ij)z (r ik) Local (using a cutoff of the type F(k 2 j ;Λ)F(k 2 k ;Λ)) At N 4 LO there are new 1 LEC s Z (r;λ) = dp (2π) 3 eip r F(p 2 ;Λ) M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 23 / 32
28 Fit of the LEC s Preliminary study Minimal model: AV18 + 3NF only from 3N contact terms Terms E 3, E 5, E 7 Terms E 5, E 7, E 1 4 Λ=2 MeV 2 χ /d.o.f = 4 c E =.654 a 2 =.652 fm E 3 =-.78 E 5 =-.143 E 7 =1.523 B( 3 H) = MeV.2 4 Λ=3 MeV 2 χ /d.o.f = 3.5 c E =.542 a 2 =.615 fm E 5 =-.262 E 7 =1.756 E 1 =-.649 B( 3 H) = MeV.2 dσ/dω 3 2 T dσ/dω 3 2 T θ (degrees) θ (degrees) θ (degrees) θ (degrees) T 2.1 T T 2.1 T θ (degrees) θ (degrees) θ (degrees) θ (degrees) i T 11 A y i T 11 A y θ (degrees) θ (degrees) θ (degrees) θ (degrees) M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 24 / 32
29 3NF effect in p 3 He scattering (1) p 3 He phase-shift - Comparison PSA/Theory (PSA: [Daniels et al., 21]) N2LO 3NF only -2 3 phase-shift S NN only NN+3N TUNL 21 phase-shift P -6 phase-shift S1 ε(1 + ) phase-shift E p [MeV] E p [MeV] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 25 / 32
30 3NF effect in p 3 He scattering (1) p 3 He phase-shift - Comparison PSA/Theory (PSA: [Daniels et al., 21]) N2LO 3NF only -2 3 phase-shift S NN only NN+3N TUNL 21 AV18/IL7 phase-shift P -6 phase-shift S1 ε(1 + ) phase-shift E p [MeV] E p [MeV] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 25 / 32
31 3NF effect in p 3 He scattering (1) p 3 He phase-shift - Comparison PSA/Theory (PSA: [Daniels et al., 21]) N2LO 3NF only -2 3 phase-shift S NN only NN+3N TUNL 21 N3LO5/N2LO5 N3LO6/N2LO6 phase-shift P -6 phase-shift S1 ε(1 + ) phase-shift E p [MeV] E p [MeV] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 25 / 32
32 3NF effect in p 3 He scattering (2) p 3 He phase-shift - Comparison PSA/Theory PSA: [Daniels et al., 21] 4 2 phase-shift P1 NN only NN+3N TUNL 21 phase-shift ε(1 - ) 5 6 phase-shift P2 P1 5 phase-shift E p [MeV] E p [MeV] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 26 / 32
33 3NF effect in p 3 He scattering (2) p 3 He phase-shift - Comparison PSA/Theory PSA: [Daniels et al., 21] 4 2 phase-shift P1 NN only NN+3N TUNL 21 AV18/IL7 phase-shift ε(1 - ) 5 6 phase-shift P2 P1 5 phase-shift E p [MeV] E p [MeV] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 26 / 32
34 3NF effect in p 3 He scattering (2) p 3 He phase-shift - Comparison PSA/Theory PSA: [Daniels et al., 21] 4 2 phase-shift P1 NN only NN+3N TUNL 21 N3LO5/N2LO5 N3LO6/N2LO6 phase-shift ε(1 - ) 5 6 phase-shift P2 P1 5 phase-shift E p [MeV] E p [MeV] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 26 / 32
35 p 3 He observables at E p = 5.54 MeV (1) 4 NN band NN+3N band 3 dσ/dω [mb/sr].5.4 A y.2 A y M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 27 / 32
36 p 3 He observables at E p = 5.54 MeV (1) 4 NN band NN+3N band AV18/IL7 3 dσ/dω [mb/sr].5.4 A y.2 A y M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 27 / 32
37 p 3 He observables at E p = 5.54 MeV (1) 4 3 NN band NN+3N band N3LO5/N2LO5 N3LO6/N2LO6 dσ/dω [mb/sr].5.4 A y.2 A y M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 27 / 32
38 p 3 He observables at E p = 5.54 MeV (2).2.2 A yy.2 A xx.1 A xz M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 28 / 32
39 S = & S = 1 n 3 He scattering lenght [fm] Int. Method a (fm) a 1 (fm) AV18 HH 7.69 i i.77 RGM 7.79 i i.66 FY 7.71 i i.82 N3LO5 HH 7.57 i i.48 FY 3.56 i.7 AGS 7.82 i i.68 N3LO5/N2LO5* HH 7.61 i i.42 N3LO5/N2LO5 HH 7.67 i i.5 N3LO6/N2LO6 HH 7.92 i i.49 Exp.[ILL-1] 7.37(58) i4.448(5) 3.278(53) i.1(2) Exp.[ILL-2] 7.46(2) 3.36(1) Exp.[NIST] 7.57(3) 3.48(2) RGM: [Hofmann & Hale, PRC 77, 442 (28)] FY: [Lazauskas et al., PRC 83, 346 (211)] AGS: [Deltuva, priv. comm.] ILL-1: [Zimmer et al., EPJA 4, 1 (22)] ILL-2: [Ketter et al., EPJA 27, 243 (26)] NIST: [Huffman et al., PRC 7, 144 (24)] From neutron interferometry at NIST [Huber et al., PRL 13, (29)] Re(a 1 a ) EXPT = 4.2(3) fm Re(a 1 a ) N3LO5/N2LO5 = 4.24 fm Re(a 1 a ) N3LO5/N2LO5 = 4.29 fm M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 29 / 32
40 Proton- 3 H scattering at low energies First monopole resonance of 4 He E = 8.2±.5 MeV, W = 27±5 kev [Walcher, 197] FY: [R. Lazauskas, 29] Monopole resonance: [Hiyama et al., 24 ] [Bacca et al., 213 ] Tension with the experimental resonance transition FF F M (q) F M 2 /4π * Koebschall et al. Frosch et al. Walcher Hiyama et al. AV18+UIX NN(N 3 LO) + 3NF(N 2 LO) q 2 [fm -2 ] 1 Balaskho (196) N3LO5/N2LO5 (only S-waves) p- 3 H elastic scattering 8 E p =.4 MeV E p =.6 MeV E p =.99 MeV dσ/dω [mb/sr] 6 4 PRELIMINARY PRELIMINARY M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 3 / 32
41 Work in progress fix the contact N 4 LO 3NF in 3N systems and see their effect in A = 4 Extension of the HH technique to treat N d breakup (in collaboration with E. Garrido - CSIC, Madrid (Spain) comparison with the benchmark calc. of [Friar et al., (1995)] PRC (in press): p d breakup: effect of the Coulomb int. Complete the study of p 3 H, n 3 He & d d scattering Extension to A > 4 Extension of the HH technique to A > 4 systems (in collaboration with M. Gattobigio - INLN, Nice (France) ) [PRA 79, (29)], [PRC 83, 241 (211)] Use of Integral Relations to compute observables (in collaboration with E. Garrido - CSIC, Madrid (Spain) & C. Romero-Redondo - TRIUMF, Vancouver (Canada) ) No need of the asymptotic part [PRA 83, 2275 (211)], [PRC 85, 141 (212)] M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 31 / 32
42 and... Thank you Sergio!!!! Australia, 1993, Kangaroo Island M. Viviani (INFN-Pisa) Few-body systems with the HH method Marciana Marina, 27/6/14 32 / 32
Few- Systems. Selected Topics in Correlated Hyperspherical Harmonics. Body. A. Kievsky
Few-Body Systems 0, 11 16 (2003) Few- Body Systems c by Springer-Verlag 2003 Printed in Austria Selected Topics in Correlated Hyperspherical Harmonics A. Kievsky INFN and Physics Department, Universita
More informationFour-nucleon scattering
Four-nucleon scattering A. Deltuva Centro de Física Nuclear da Universidade de Lisboa Hamiltonian H + i> j 4N scattering v i j 1 v 12 4 3 2 Wave function: Schrödinger equation (HH + Kohn VP) [M. Viviani,
More informationLocal chiral NN potentials and the structure of light nuclei
Local chiral NN potentials and the structure of light nuclei Maria Piarulli @ELBA XIV WORKSHOP June 7-July 1 16, Marciana Marina, Isola d Elba PHYSICAL REVIEW C 91, 43(15) Minimally nonlocal nucleon-nucleon
More informationVariatonal description of continuum states
Variatonal description of continuum states A. Kievsky INFN, Sezione di Pisa (Italy) Collaborators Three-body systems in reactions with rare isotopes ECT*, October 2016 M. Viviani, L.E. Marcucci - INFN
More informationTheoretical studies of muon capture on light nuclei
Theoretical studies of muon capture on light nuclei Dipartimento di Fisica E. Fermi, Università di Pisa INFN, Sezione di Pisa I-56127 Pisa, Italy E-mail: laura.marcucci@df.unipi.it We review the present
More informationWeakly-Bound Systems in Atomic and Nuclear Physics March 2010
Electroweak properties of Weakly- Bound Light Nuclei Weakly-Bound Systems in Atomic and Nuclear Physics March 2010 INSTITUTE FOR NUCLEAR THEORY Collaborators Sonia Bacca Winfried Leidemann, Giuseppina
More informationModern Theory of Nuclear Forces
Evgeny Epelbaum, FZ Jülich & University Bonn Lacanau, 29.09.2009 Modern Theory of Nuclear Forces Lecture 1: Lecture 2: Lecture 3: Introduction & first look into ChPT EFTs for two nucleons Nuclear forces
More informationFew 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
More informationApplication of few-nucleon physics in astrophysics
Journal of Physics: Conference Series PAPER OPEN ACCESS Application of few-nucleon physics in astrophysics To cite this article: Michele Viviani and Laura Elisa Marcucci 2016 J. Phys.: Conf. Ser. 703 012013
More informationEvgeny 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:
More informationMuon capture on A = 2 and 3 nuclei
Available online at www.sciencedirect.com Physics Procedia 17 (2011) 145 152 Physics of Fundamental Symmetries and Interactions - PSI2010 Muon capture on A = 2 and 3 nuclei L.E. Marcucci Department of
More information(March 12, 1999) Abstract. The Kohn variational principle and the (correlated) Hyperspherical Harmonics
Neutron 3 H and Proton 3 He Zero Energy Scattering M. Viviani 1, S. Rosati 1,2 and A. Kievsky 1, 1 Istituto Nazionale di Fisica Nucleare, Piazza Torricelli 2, 56100 Pisa, Italy 2 Dipartimento di Fisica,
More informationThe nucleon-nucleon system in chiral effective theory
The nucleon-nucleon system in chiral effective theory Daniel Phillips Ohio University Research supported by the US Department of Energy Plan χet for nuclear forces: the proposal Leading order for S waves
More informationProton deuteron elastic scattering above the deuteron breakup
Proton deuteron elastic scattering above the deuteron breakup A. Kievsky, S. Rosati and M. Viviani Istituto Nazionale di Fisica Nucleare, Via Buonarroti 2, 56100 Pisa, Italy Dipartimento di Fisica, Via
More informationNuclear Forces - Lecture 6 -
Physics Department, Tohoku University, June 30 July 2, 2014 Nuclear Forces - Lecture 6 - Nuclear many-body forces from chiral EFT R. Machleidt University of Idaho 1 Nuclear Forces - Overview of all lectures
More informationAb initio lattice EFT from light to medium mass nuclei Nuclear Lattice EFT Collaboration
Ab initio lattice EFT from light to medium mass nuclei Nuclear Lattice EFT Collaboration Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Timo Lähde (Jülich) Dean Lee (NC State) Thomas Luu (Jülich/Bonn)
More informationQuantum Monte Carlo calculations of medium mass nuclei
Quantum Monte Carlo calculations of medium mass nuclei Diego Lonardoni FRIB Theory Fellow In collaboration with: J. Carlson, LANL S. Gandolfi, LANL X. Wang, Huzhou University, China A. Lovato, ANL & UniTN
More informationStudy of nucleonic matter with a consistent twoand three-body perturbative chiral interaction
Journal of Physics: Conference Series OPEN ACCESS Study of nucleonic matter with a consistent twoand three-body perturbative chiral interaction To cite this article: L Coraggio et al 2014 J. Phys.: Conf.
More informationModern Theory of Nuclear Forces
Evgeny Epelbaum PAX Meeting, Stockholm, 15.06.2010 Modern Theory of Nuclear Forces Evgeny Epelbaum, Ruhr-Universität Bochum Outline Chiral EFT for nuclear forces Some hot topics (work in progress) Deuteron
More informationNuclear matter calculations with chiral interactions
INFN, Sezione di Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy E-mail: domenico.logoteta@pi.infn.it Ignazio Bombaci Dipartimento di Fisica, Universitá di Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa,
More informationChiral effective field theory on the lattice: Ab initio calculations of nuclei
Chiral effective field theory on the lattice: Ab initio calculations of nuclei Nuclear Lattice EFT Collaboration Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Timo Lähde (Jülich) Dean Lee (NC State)
More informationCoupled-cluster computations of weak decays in nuclei
Coupled-cluster computations of weak decays in nuclei Gaute Hagen Oak Ridge National Laboratory Nuclear ab initio Theories and Neutrino Physics INT, March 6th, 2018 Trend in realistic ab-initio calculations
More informationThree- and four-particle scattering
Three- and four-particle scattering A. Deltuva Centro de Física Nuclear da Universidade de Lisboa Few-particle scattering Three-particle scattering equations Three-nucleon system Three-body direct nuclear
More informationThree-nucleon forces and neutron-rich nuclei
Three-nucleon forces and neutron-rich nuclei Achim Schwenk Facets of Strong Interaction Physics Hirschegg 40 + Bengt 60, Jan. 18, 2012 Happy Birthday Bengt! Outline Understanding three-nucleon forces Three-body
More informationarxiv: v1 [nucl-th] 3 Feb 2014
Study of nucleonic matter with a consistent two- and three-body perturbative chiral interaction arxiv:1402.0380v1 [nucl-th] 3 Feb 2014 L Coraggio 1, J W Holt 2, N Itaco 1,3, R Machleidt 4, L E Marcucci
More informationThe 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.
More informationLight Nuclei from chiral EFT interactions
Light Nuclei from chiral EFT interactions Petr Navratil Lawrence Livermore National Laboratory* Collaborators: V. G. Gueorguiev (UCM), J. P. Vary (ISU), W. E. Ormand (LLNL), A. Nogga (Julich), S. Quaglioni
More informationQuantum Monte Carlo calculations of neutron and nuclear matter
Quantum Monte Carlo calculations of neutron and nuclear matter Stefano Gandolfi Los Alamos National Laboratory (LANL) Advances and perspectives in computational nuclear physics, Hilton Waikoloa Village,
More informationINTERACTIONS, CURRENTS, AND THE STRUCTURE OF FEW-NUCLEON SYSTEMS
INTERACTIONS, CURRENTS, AND THE STRUCTURE OF FEW-NUCLEON SYSTEMS R. SCHIAVILLA Jefferson Lab, Newport News, VA 23606 and Old Dominion University, Norfolk, VA 23529 arxiv:nucl-th/0010061 18 Oct 2000 Our
More informationBRIDGING OVER p-wave π-production AND WEAK PROCESSES IN FEW-NUCLEON SYSTEMS WITH CHIRAL PERTURBATION THEORY
MENU 2007 11th International Conference on Meson-Nucleon Physics and the Structure of the Nucleon September10-14, 2007 IKP, Forschungzentrum Jülich, Germany BRIDGING OVER p-wave π-production AND WEAK PROCESSES
More informationA path to lepton-nucleus reactions from first principles
Canada s National Laboratory for Particle and Nuclear Physics Laboratoire national canadien pour la recherche en physique nucléaire et en physique des particules A path to lepton-nucleus reactions from
More informationTowards first-principle description of electromagnetic reactions in medium-mass nuclei
Canada s National Laboratory for Particle and Nuclear Physics Laboratoire national canadien pour la recherche en physique nucléaire et en physique des particules Towards first-principle description of
More informationNuclear and Nucleon Matter Constraints on Three-Nucleon Forces
Nuclear and Nucleon Matter Constraints on Three-Nucleon Forces Robert B. Wiringa, Physics Division, Argonne National Laboratory Joe Carlson, Los Alamos Stefano Gandolfi, Los Alamos Alessandro Lovato, Argonne
More informationAFDMC Method for Nuclear Physics and Nuclear Astrophysics
AFDMC Method for Nuclear Physics and Nuclear Astrophysics Thanks to INFN and to F. Pederiva (Trento) Outline Motivations: NN scattering data few body theory. Few-body many body experiments/observations?
More informationarxiv: v1 [nucl-th] 20 Jun 2016
Local chiral potentials and the structure of light nuclei M. Piarulli a, L. Girlanda b,c, R. Schiavilla d,e, A. Kievsky f, A. Lovato a, L.E. Marcucci g,f, Steven C. Pieper a, M. Viviani f, and R.B. Wiringa
More informationNuclear Physics from Lattice Effective Field Theory
Nuclear Physics from Lattice Effective Field Theory Dean Lee (NCSU/Bonn) work done in collaboration with Evgeny Epelbaum (Bochum) Hermann Krebs (Bochum) Ulf-G. Meißner (Bonn/Jülich) Buḡra Borasoy (now
More informationNeutron-rich matter and neutrino-matter interactions based on chiral effective field theory
Neutron-rich matter and neutrino-matter interactions based on chiral effective field theory Achim Schwenk Astrophysical Transients: Multi-Messenger Probes of Nuclear Physics INT, July 29, 2011 Outline
More informationNeutrino processes in supernovae from chiral EFT
Neutrino processes in supernovae from chiral EFT Achim Schwenk CANADA S NATIONAL LABORATORY FOR PARTICLE AND NUCLEAR PHYSICS Owned and operated as a joint venture by a consortium of Canadian universities
More informationElectromagnetic Response of Light Nuclei with Integral Transforms
Electromagnetic Response of Light Nuclei with Integral Transforms LIT method Low-energy continuum observables with LIT Resonances S-Factor in presence of Coulomb potential Electron scattering at q 500
More informationQuantum Monte Carlo calculations with chiral Effective Field Theory Interactions
Quantum Monte Carlo calculations with chiral Effective Field Theory Interactions Alexandros Gezerlis East Lansing, MI 3rd International Symposium on Nuclear Symmetry Energy July 25, 2013 Motivation for
More informationNuclear few- and many-body systems in a discrete variable representation basis
Nuclear few- and many-body systems in a discrete variable representation basis Jeremy W. Holt* Department of Physics University of Washington *with A. Bulgac, M. M. Forbes L. Coraggio, N. Itaco, R. Machleidt,
More informationThe NN system: why and how we iterate
The NN system: why and how we iterate Daniel Phillips Ohio University Research supported by the US department of energy Plan Why we iterate I: contact interactions Why we iterate II: pion exchange How
More information(Todays) Progress in coupled cluster compuations of atomic nuclei
(Todays) Progress in coupled cluster compuations of atomic nuclei Gaute Hagen Oak Ridge National Laboratory Progress in Ab Initio Techniques in Nuclear Physics TRIUMF, February 26 th, 2019 Collaborators
More informationAb initio alpha-alpha scattering using adiabatic projection method
Ab initio alpha-alpha scattering using adiabatic projection method Serdar Elhatisari Advances in Diagrammatic Monte Carlo Methods for QFT Calculations in Nuclear-, Particle-, and Condensed Matter Physics
More informationNuclear structure from chiral-perturbation-theory two- plus three-nucleon interactions
Nuclear structure from chiral-perturbation-theory two- plus three-nucleon interactions Petr Navratil Lawrence Livermore National Laboratory* Collaborators: W. E. Ormand (LLNL), J. P. Vary (ISU), E. Caurier
More informationTHE THREE NUCLEON SYSTEM AT LEADING ORDER OF CHIRAL EFFECTIVE THEORY
THE THREE NUCLEON SYSTEM AT LEADING ORDER OF CHIRAL EFFECTIVE THEORY Young-Ho Song(RISP, Institute for Basic Science) Collaboration with R. Lazauskas( IPHC, IN2P3-CNRS) U. van Kolck (Orsay, IPN & Arizona
More informationNuclear 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
More informationRG & EFT for nuclear forces
RG & EFT for nuclear forces Andreas Nogga, Forschungszentrum Jülich ECT* school, Feb/March 2006 Low momentum interactions: Using the RG to simplify the nuclear force for many-body calculations. Application
More informationManifestations of Neutron Spin Polarizabilities in Compton Scattering on d and He-3
Manifestations of Neutron Spin Polarizabilities in Compton Scattering on d and He- Deepshikha Choudhury (Collaborators: D. Phillips,. Nogga, R. Hildebrandt) Supported by US-DOE Focus Neutron Spin Polarizabilities
More informationPOWER COUNTING WHAT? WHERE?
POWER COUNTING WHAT? WHERE? U. van Kolck Institut de Physique Nucléaire d Orsay and University of Arizona Supported by CNRS and US DOE 1 Outline Meeting the elephant What? Where? Walking out of McDonald
More informationParity-Violating Effects in Few-Nucleon Systems
Parity-Violating Effects in Few-Nucleon Systems Joe Carlson (LANL) Rocco Schiavilla (JLAB/ODU) Alejandro Kievsky (INFN-Pisa) Laura Marcucci (U-Pisa) Michele Viviani (INFN-Pisa) Mark Paris (JLAB) Ben Gibson
More informationQuantum Monte Carlo calculations of two neutrons in finite volume
Quantum Monte Carlo calculations of two neutrons in finite volume Philipp Klos with J. E. Lynn, I. Tews, S. Gandolfi, A. Gezerlis, H.-W. Hammer, M. Hoferichter, and A. Schwenk Nuclear Physics from Lattice
More informationAb Initio Calculations of Charge Symmetry Breaking in Light Hypernuclei
Ab Initio Calculations of Charge Symmetry Breaking in Light Hypernuclei Daniel Gazda Nuclear Physics Institute Prague, Czech Republic Together with: A. Gal (HU Jerusalem) Outline Introduction Charge symmetry
More informationNuclear physics around the unitarity limit
Nuclear physics around the unitarity limit Sebastian König Nuclear Theory Workshop TRIUMF, Vancouver, BC February 28, 2017 SK, H.W. Grießhammer, H.-W. Hammer, U. van Kolck, arxiv:1607.04623 [nucl-th] SK,
More informationLattice Simulations with Chiral Nuclear Forces
Lattice Simulations with Chiral Nuclear Forces Hermann Krebs FZ Jülich & Universität Bonn July 23, 2008, XQCD 2008, NCSU In collaboration with B. Borasoy, E. Epelbaum, D. Lee, U. Meißner Outline EFT and
More informationNucleon Nucleon Forces and Mesons
Canada s ational Laboratory for Particle and uclear Physics Laboratoire national canadien pour la recherche en physique nucléaire et en physique des particules ucleon ucleon Forces and Mesons Sonia Bacca
More informationWeak reactions with light nuclei
Weak reactions with light nuclei Nir Barnea, Sergey Vaintraub The Hebrew University Doron Gazit INT, University of Washington Eilat, November 9-14, 2008 Nir Barnea (HUJI) Weak reactions with light nuclei
More informationUniversality in Four-Boson Systems
Universality in Four-Boson Systems M. R. Hadizadeh INPP, Department of Physics & Astronomy, Ohio University hadizadm@ohio.edu Work done in collaboration with: M.T. Yamashita & L. Tomio (UNESP), A. Delfino
More informationNuclear 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,
More informationMICROSCOPIC OPTICAL POTENTIAL FROM NN CHIRAL POTENTIALS. Carlotta Giusti Università and INFN, Pavia. Matteo Vorabbi (TRIUMF) Paolo Finelli (Bologna)
MICROSCOPIC OPTICAL POTENTIAL FROM NN CHIRAL POTENTIALS Carlotta Giusti Università and INFN, Pavia Matteo Vorabbi (TRIUMF) Paolo Finelli (Bologna) Nuclear ab initio Theories and Neutrino Physics: INT Seattle
More informationWeak and rare nuclear processes. Doron Gazit
Weak and rare nuclear processes Doron Gazit Outline The role of theory in calculating rare nuclear processes. Calculating weak reactions in chiral EFT. Gamow-Teller transitions within chiral EFT: from
More informationThree-cluster dynamics within an ab initio framework
Three-cluster dynamics within an ab initio framework Universality in Few-Body Systems: Theoretical Challenges and New Directions INT 14-1, March 26, 2014 S. Quaglioni Collaborators: C. Romero-Redondo (TRIUMF)
More informationModern Theory of Nuclear Forces
Evgeny Epelbaum, FZ Jülich & University Bonn Lacanau, 28.09.2009 Modern Theory of Nuclear Forces Lecture 1: Lecture 2: Introduction & first look into ChPT EFTs for two nucleons Chiral Perturbation Theory
More informationApplications of Renormalization Group Methods in Nuclear Physics 2
Applications of Renormalization Group Methods in Nuclear Physics 2 Dick Furnstahl Department of Physics Ohio State University HUGS 2014 Outline: Lecture 2 Lecture 2: SRG in practice Recap from lecture
More informationg A Quenching Information from Neutrino Scattering
g A Quenching Information from Neutrino Scattering Saori Pastore νeclipse Workshop Knoxville, TN, August 2017 Open Questions in Fundamental Symmetries and Neutrino Physics Majorana Neutrinos, Neutrinos
More informationarxiv:nucl-th/ v1 22 Sep 2000
1 arxiv:nucl-th/967v1 22 Sep 2 Chiral Dynamics in Few Nucleon Systems E. Epelbaum a, H. Kamada a,b, A. Nogga b, H. Wita la c, W. Glöckle b, and Ulf-G. Meißner a a Forschungszentrum Jülich, Institut für
More informationCoupled-cluster theory for nuclei
Coupled-cluster theory for nuclei Thomas Papenbrock and G. Hagen D. J. Dean M. Hjorth-Jensen B. Velamur Asokan INT workshop Weakly-bound systems in atomic and nuclear physics Seattle, March 8-12, 2010
More informationElectromagnetic reactions from few to many-body systems Giuseppina Orlandini
Electromagnetic reactions from few to many-body systems Giuseppina Orlandini ECT* Workshop on Recent advances and challenges in the description of nuclear reactions at the limit of stability, March 5-9,
More informationQuantum Monte Carlo calculations of the equation of state of neutron matter with chiral EFT interactions
Quantum Monte Carlo calculations of the equation of state of neutron matter with chiral EFT interactions Ingo Tews (Institute for Nuclear Theory Seattle) In collaboration with A.Gezerlis, J. Carlson, S.
More informationSciDAC project NUCLE lead PI: Joe Carlson (LA PetaApps award lead PI: Jerry Draayer (L. lead PI: James P Vary (I NERSC
Emer in light nucl NCSM and neutrinoless double beta decay James P. Vary, Iowa State University INT/Topical Collaboration Workshop Seattle, Washington, June 20-21, 2017 Neutrinos and Fundamental Symmetries
More informationThe oxygen anomaly F O
The oxygen anomaly O F The oxygen anomaly - not reproduced without 3N forces O F without 3N forces, NN interactions too attractive many-body theory based on two-nucleon forces: drip-line incorrect at 28
More informationRG & EFT for nuclear forces
RG & EFT for nuclear forces Andreas Nogga, Forschungszentrum Jülich ECT* school, Feb/March 2006 Low momentum interactions: Using the RG to simplify the nuclear force for many-body calculations. Application
More informationCoupled-cluster theory for medium-mass nuclei
Coupled-cluster theory for medium-mass nuclei Thomas Papenbrock and G. Hagen (ORNL) D. J. Dean (ORNL) M. Hjorth-Jensen (Oslo) A. Nogga (Juelich) A. Schwenk (TRIUMF) P. Piecuch (MSU) M. Wloch (MSU) Seattle,
More informationNucleon-nucleon interaction in covariant chiral effective field theory
Guilin, China The Seventh Asia-Pacific Conference on Few-Body Problems in Physics Nucleon-nucleon interaction in covariant chiral effective field theory Xiu-Lei Ren School of Physics, Peking University
More informationNovel NN interaction and the spectroscopy of light nuclei
Physics Letters B 621 (2005) 96 101 www.elsevier.com/locate/physletb Novel NN interaction and the spectroscopy of light nuclei A.M. Shirokov a,j.p.vary b, A.I. Mazur c,s.a.zaytsev c,t.a.weber b a Skobeltsyn
More informationTheoretical Optical Potential Derived From Chiral Potentials
NUCLEAR THERY, Vol. 35 (206) eds. M. Gaidarov, N. Minkov, Heron Press, Sofia Theoretical ptical Potential Derived From Chiral Potentials M. Vorabbi,2, P. Finelli 3, C. Giusti 2 TRIUMF, 4004 Wesbrook Mall,
More informationAlex Gezerlis. New Ideas in Constraining Nuclear Forces ECT*, Trento, Italy June 5, 2018
Quantum Monte Carlo interactions with From microscopic to effective Chiral Effective Field Theory Interactions using Quantum Monte Carlo Alex Gezerlis New Ideas in Constraining Nuclear Forces ECT*, Trento,
More informationLight hypernuclei based on chiral and phenomenological interactions
Mitglied der Helmholtz-Gemeinschaft Light hypernuclei based on chiral and phenomenological interactions Andreas Nogga, Forschungszentrum Jülich International Conference on Hypernuclear and Strange Particle
More informationNuclear Structure and Reactions using Lattice Effective Field Theory
Nuclear Structure and Reactions using Lattice Effective Field Theory Dean Lee North Carolina State University Nuclear Lattice EFT Collaboration Frontiers of Nuclear Physics Kavli Institute for Theoretical
More informationhg: 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
More informationRecent results in lattice EFT for nuclei
Recent results in lattice EFT for nuclei Dean Lee (NC State) Nuclear Lattice EFT Collaboration Centro de Ciencias de Benasque Pedro Pascua Bound states and resonances in EFT and Lattice QCD calculations
More informationRenormalization 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
More informationBayesian 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)
More informationNuclei as Bound States
Nuclei as Bound States Lecture 1: Hamiltonian Robert Roth Overview Lecture 1: Hamiltonian Prelude Nuclear Hamiltonian Matrix Elements Two-Body Problem Correlations & Unitary Transformations Lecture 2:
More informationOverview of low energy NN interaction and few nucleon systems
1 Overview of low energy NN interaction and few nucleon systems Renato Higa Theory Group, Jefferson Lab Cebaf Center, A3 (ext6363) higa@jlaborg Lecture II Basics on chiral EFT π EFT Chiral effective field
More informationThree-nucleon potentials in nuclear matter. Alessandro Lovato
Three-nucleon potentials in nuclear matter Alessandro Lovato PRC 83, 054003 (2011) arxiv:1109.5489 Outline Ab initio many body method Nuclear Hamiltonian: 2- and 3- body potentials Density dependent potential
More informationAb Initio Nuclear Structure Theory
Ab Initio Nuclear Structure Theory Lecture 1: Hamiltonian Robert Roth Overview Lecture 1: Hamiltonian Prelude Many-Body Quantum Mechanics Nuclear Hamiltonian Matrix Elements Lecture 2: Correlations Two-Body
More informationPionless EFT for Few-Body Systems
Pionless EFT for Few-Body Systems Betzalel Bazak Physique Theorique Institut de Physique Nucleaire d Orsay Nuclear Physics from Lattice QCD Insitute for Nuclear Theory April 7, 2016 Seattle Betzalel Bazak
More informationEffective Field Theories in Nuclear and Hadron Physics
Effective Field Theories in Nuclear and Hadron Physics Vadim Lensky Theoretical Physics Group, The University of Manchester January 11, 2013 V. Lensky EFTs in Hadron and Nuclear Physics 1 Outline Introduction
More informationarxiv: v1 [nucl-th] 5 Jan 2019
What is wrong with our current nuclear forces? R. Machleidt Department of Physics, University of Idaho, Moscow, Idaho 83844, USA Abstract arxiv:1901.01473v1 [nucl-th] 5 Jan 2019 I discuss ab initio predictions
More informationConstraints on neutron stars from nuclear forces
Constraints on neutron stars from nuclear forces Achim Schwenk Workshop on the formation and evolution of neutron stars Bonn, Feb. 27, 2012 Main points Advances in nuclear forces and nuclear matter theory
More informationThe No Core Shell Model: Its Formulation, Application and Extensions. Bruce R. Barrett University of Arizona,
The No Core Shell Model: Its Formulation, Application and Extensions Bruce R. Barrett University of Arizona, Tucson, INT Spring Program 2011 March 23, 2011 MICROSCOPIC NUCLEAR-STRUCTURE THEORY 1. Start
More informationNuclear electromagnetic charge and current operators in ChEFT
Nuclear electromagnetic carge and current operators in CEFT Luca Girlanda Università del Salento & INFN Lecce collaborators: Saori Pastore, Bob Wiringa (ANL), Rocco Sciavilla, (Jlab), Laura Marcucci, Alejandro
More informationScattering and reactions in Quantum Monte Carlo. Ken Nollett Argonne 23 July 2004 p-shell workshop
Scattering and reactions in Quantum Monte Carlo Ken Nollett Argonne 23 July 2004 p-shell workshop It would be nice if nuclear properties could be predicted with confidence from basic principles, particularly
More informationThree-Nucleon Forces and Masses of Neutron-Rich Nuclei Jason D. Holt
Three-Nucleon Forces and Masses of Neutron-Rich Nuclei Jason D. Holt Drip Lines and Magic Numbers: The Evolving Nuclear Landscape 3N forces important in light nuclei, nuclear matter What are the limits
More informationStatus of deuteron stripping reaction theories
Status of deuteron stripping reaction theories Pang Danyang School of Physics and Nuclear Energy Engineering, Beihang University, Beijing November 9, 2015 DY Pang Outline 1 Current/Popular models for (d,
More informationFate of the neutron-deuteron virtual state as an Efimov level
Fate of the neutron-deuteron virtual state as an Efimov level Gautam Rupak Collaborators: R. Higa (USP), A. Vaghani (MSU), U. van Kolck (IPN-Orsay/UA) Jefferson Laboratory Theory Seminar, Mar 19, 2018
More informationarxiv:nucl-th/ v1 16 Jul 2002
Evolution of Nuclear Spectra with Nuclear Forces R. B. Wiringa[*] and Steven C. Pieper[ ] Physics Division, Argonne National Laboratory, Argonne, IL 60439 (Dated: February 8, 2008) We first define a series
More informationNuclear electric dipole moment in the Gaussian expansion method
Nuclear electric dipole moment in the Gaussian expansion method Nodoka Yamanaka (ithes Group, RIKEN) In collaboration with E. Hiyama (RIKEN), T. Yamada (Kanto-Gakuin Univ.), Y. Funaki (RIKEN) 2015/10/12
More informationEffective Field Theory for light nuclear systems
Effective Field Theory for light nuclear systems Jimmy Rotureau Chalmers University of Technology, Göteborg, Sweden B. Barrett, University of Arizona, Tucson I. Stetcu, University of Washington, Seattle
More information