probing effect of tensor interactions in nuclei via p d
play

Probing effect of tensor interactions in nuclei via (p, d) reaction - PowerPoint PPT Presentation

Dec 10, 2023 •170 likes •518 views

Probing effect of tensor interactions in nuclei via (p, d) reaction Guo Chenlei (On behalf of RCNP-E396) Research Center of Nuclear Science and Technology ( RCNST ) Beihang University C.L. Guo 1 Contents Physics Motivation ( Already

  1. Probing effect of tensor interactions in nuclei via (p, d) reaction Guo Chenlei (On behalf of RCNP-E396) Research Center of Nuclear Science and Technology ( RCNST ) Beihang University C.L. Guo 1

  2. Contents  Physics Motivation ( Already talked a lot in this symposium… )  Experiments in RCNP, Osaka  Preliminary results & Discussion  Summary & Acknowledgments Contents C.L. Guo 2

  3. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Experiments in RCNP C.L. Guo 3

  4. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Experiments in RCNP C.L. Guo 3

  5. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Further question has been asked: reaction mechanism effect at finite angle Experiments in RCNP C.L. Guo 3

  6. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Experiments in RCNP C.L. Guo 3

  7. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Configuration difference for 16 O & 12 C 16 O 2s 1/2 12 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 proton neutron proton neutron Experiments in RCNP C.L. Guo 4

  8. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Configuration difference for 16 O & 12 C 15 O 2s 1/2 12 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 proton neutron proton neutron 15 O: negative parity ground state ( J π =1/2- ) Experiments in RCNP C.L. Guo 4

  9. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Configuration difference for 16 O & 12 C 15 O 2s 1/2 12 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 proton neutron proton neutron 15 O: negative parity ground state ( J π =1/2- ) negative parity excited state ( J π =3/2- ) Experiments in RCNP C.L. Guo 4

  10. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Configuration difference for 16 O & 12 C 15 O 2s 1/2 11 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 proton neutron proton neutron 11 C: negative parity ground state ( J π =3/2- ) 15 O: negative parity ground state ( J π =1/2- ) negative parity excited state ( J π =3/2- ) Experiments in RCNP C.L. Guo 4

  11. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Configuration difference for 16 O & 12 C 15 O 2s 1/2 11 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 proton neutron proton neutron 11 C: negative parity ground state ( J π =3/2- ) negative parity excited state ( J π =1/2- ) 15 O: negative parity ground state ( J π =1/2- ) negative parity excited state ( J π =3/2- ) Experiments in RCNP C.L. Guo 4

  12. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Tensor selection rule: Configuration difference for 16 O & 12 C ∆ L=2, ∆ s=2, ∆ J=0 16 O 2s 1/2 12 C 1d 5/2 π 1p 1/2 π 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 proton neutron proton neutron Experiments in RCNP C.L. Guo 4

  13. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Tensor selection rule: Configuration difference for 16 O & 12 C ∆ L=2, ∆ s=2, ∆ J=0 16 O 2s 1/2 12 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 Ground state of 12 C (J π =0 + ): Ground state of 16 O (J π =0 + ): mixing of 2p-2h configuration mixing of 2p-2h configuration Experiments in RCNP C.L. Guo 4

  14. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Tensor selection rule: Configuration difference for 16 O & 12 C ∆ L=2, ∆ s=2, ∆ J=0 15 O 2s 1/2 12 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 Ground state of 12 C (J π =0 + ): Ground state of 16 O (J π =0 + ): mixing of 2p-2h configuration mixing of 2p-2h configuration → 15 O: positive parity excited state ( J π =5/2+ ) Experiments in RCNP C.L. Guo 4

  15. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Tensor selection rule: Configuration difference for 16 O & 12 C ∆ L=2, ∆ s=2, ∆ J=0 15 O 2s 1/2 11 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 Ground state of 12 C (J π =0 + ): Ground state of 16 O (J π =0 + ): mixing of 2p-2h configuration mixing of 2p-2h configuration → 11 C: ground state ( J π =3/2- ) → 15 O: positive parity excited state ( J π =5/2+ ) Experiments in RCNP C.L. Guo 4

  16. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Tensor selection rule: Configuration difference for 16 O & 12 C ∆ L=2, ∆ s=2, ∆ J=0 15 O 2s 1/2 11 C 1d 5/2 1p 1/2 1p 1/2 1p 3/2 1p 3/2 1s 1/2 1s 1/2 Ground state of 12 C (J π =0 + ): Ground state of 16 O (J π =0 + ): mixing of 2p-2h configuration mixing of 2p-2h configuration → 11 C: ground state ( J π =3/2- ) → 15 O: positive parity excited state ( J π =5/2+ ) excited state ( J π =1/2- ) Experiments in RCNP C.L. Guo 4

  17. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Grand RAIDEN Spectrometer p/ Δ p ~37000 Scattering angle: 0 o ~ 10 10 o 16 O target: Mylar (C 10 H 8 O 4 ) 12 C target: CD 2 Beam energy: 392 MeV/nucleon Focal Plane Detector: Two Plastic scintillator for Δ E & TOF Beam Intensity: 10 nA Energy resolution ≤ 150keV (Achromatic mode) Two VDCs (drift chamber) for position and angle (x,dx,y,dy) Experiments in RCNP C.L. Guo 5

  18. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Grand RAIDEN Spectrometer p/ Δ p ~37000 Scattering angle: 0 o ~ 10 10 o 16 O target: Mylar (C 10 H 8 O 4 ) 12 C target: CD 2 Beam energy: 392 MeV/nucleon Focal Plane Detector: Two Plastic scintillator for Δ E & TOF Beam Intensity: 10 nA Energy resolution ≤ 150keV (Achromatic mode) Two VDCs (drift chamber) for position and angle (x,dx,y,dy) Experiments in RCNP C.L. Guo 5

  19. Nucleon pick-up reaction( 12 C(p,d) & 16 O(p,d) ) @ RCNP, Osaka Grand RAIDEN Spectrometer p/ Δ p ~37000 Scattering angle: 0 o ~ 10 10 o 16 O target: Mylar (C 10 H 8 O 4 ) 12 C target: CD 2 Beam energy: 392 MeV/nucleon Focal Plane Detector: Two Plastic scintillator for Δ E & TOF Beam Intensity: 10 nA Energy resolution ≤ 150keV (Achromatic mode) Two VDCs (drift chamber) for position and angle (x,dx,y,dy) Experiments in RCNP C.L. Guo 5

  20. 16 O(p,d) 15 O: 1/2- 18.5MeV: Phys. Rev. 129, 272 (1963) 19MeV: Phys. Rev. 129, 272 (1963) 30.3MeV: Nucl. Phys. A 99, 669 (1967) 45MeV: Phys. Rev. 187, 1246 (1969) 65MeV: Nucl. Phys. A 255, 187 (1975) 100MeV: Nucl. Phys. A 106, 357 (1968) 200MeV: Phys. Rev. C 39, 65 (1989) 800MeV: Phys. Rev. C 30, 593 (1984) E314 198MeV & 295MeV & 392MeV: Phys. Lett. B 725, 277 (2013) Preliminary results and discussion C.L. Guo 6

  21. 16 O(p,d) 15 O: 1/2- 16 O(p,d) 15 O: 5/2+ 18.5MeV: Phys. Rev. 129, 272 (1963) 19MeV: Phys. Rev. 129, 272 (1963) 30.3MeV: Nucl. Phys. A 99, 669 (1967) 45MeV: Phys. Rev. 187, 1246 (1969) 65MeV: Nucl. Phys. A 255, 187 (1975) 100MeV: Nucl. Phys. A 106, 357 (1968) 200MeV: Phys. Rev. C 39, 65 (1989) 800MeV: Phys. Rev. C 30, 593 (1984) E314 198MeV & 295MeV & 392MeV: Phys. Lett. B 725, 277 (2013) Preliminary results and discussion C.L. Guo 6

  22. 16 O(p,d) 15 O: 1/2- 16 O(p,d) 15 O: 5/2+ 16 O(p,d) 15 O: 3/2- 18.5MeV: Phys. Rev. 129, 272 (1963) 19MeV: Phys. Rev. 129, 272 (1963) 30.3MeV: Nucl. Phys. A 99, 669 (1967) 45MeV: Phys. Rev. 187, 1246 (1969) 65MeV: Nucl. Phys. A 255, 187 (1975) 100MeV: Nucl. Phys. A 106, 357 (1968) 200MeV: Phys. Rev. C 39, 65 (1989) 800MeV: Phys. Rev. C 30, 593 (1984) E314 198MeV & 295MeV & 392MeV: Phys. Lett. B 725, 277 (2013) Preliminary results and discussion C.L. Guo 6

  23. 12 C(p,d) 11 C: 3/2- 30.3MeV: Nucl. Phys. A 99, 669 (1967) 51.93MeV: J. Phys. Journal 48, 1812 (1980) 61MeV: Phys. Rev. C 8,1045 (1973) 65MeV: Nucl. Phys. A 255, 187 (1975) 100MeV: Nucl. Phys. A 106, 357 (1968) 800MeV: Phys. Rev. C 30, 593 (1984) E314 198MeV & 295MeV & 392MeV: Phys. Lett. B 725, 277 (2013) Preliminary results and discussion C.L. Guo 6

  24. 12 C(p,d) 11 C: 3/2- 16 O(p,d) 15 O:1/2- 12 C(p,d) 11 C: ½- 30.3MeV: Nucl. Phys. A 99, 669 (1967) 51.93MeV: J. Phys. Journal 48, 1812 (1980) 61MeV: Phys. Rev. C 8,1045 (1973) 65MeV: Nucl. Phys. A 255, 187 (1975) 100MeV: Nucl. Phys. A 106, 357 (1968) 800MeV: Phys. Rev. C 30, 593 (1984) E314 198MeV & 295MeV & 392MeV: Phys. Lett. B 725, 277 (2013) Preliminary results and discussion C.L. Guo 6

  25. 12 C(p,d) 11 C: 3/2- 16 O(p,d) 15 O:1/2- 12 C(p,d) 11 C: 1/2- 12 C(p,d) 11 C: 5/2- 30.3MeV: Nucl. Phys. A 99, 669 (1967) 51.93MeV: J. Phys. Journal 48, 1812 (1980) 61MeV: Phys. Rev. C 8,1045 (1973) 65MeV: Nucl. Phys. A 255, 187 (1975) 100MeV: Nucl. Phys. A 106, 357 (1968) 800MeV: Phys. Rev. C 30, 593 (1984) E314 198MeV & 295MeV & 392MeV: Phys. Lett. B 725, 277 (2013) Preliminary results and discussion C.L. Guo 6

  26. 12 C(p,d) 11 C: 3/2- 16 O(p,d) 15 O:1/2- 12 C(p,d) 11 C: 1/2- 12 C(p,d) 11 C: 5/2- 12 C(p,d) 11 C: 3/2- 30.3MeV: Nucl. Phys. A 99, 669 (1967) 51.93MeV: J. Phys. Journal 48, 1812 (1980) 61MeV: Phys. Rev. C 8,1045 (1973) 65MeV: Nucl. Phys. A 255, 187 (1975) 100MeV: Nucl. Phys. A 106, 357 (1968) 800MeV: Phys. Rev. C 30, 593 (1984) E314 198MeV & 295MeV & 392MeV: Phys. Lett. B 725, 277 (2013) Preliminary results and discussion C.L. Guo 6

Recommend

Light Nuclei from chiral chiral EFT interactions EFT interactions Light Nuclei from Petr

Light Nuclei from chiral chiral EFT interactions EFT interactions Light Nuclei from Petr

Light Nuclei from chiral chiral EFT interactions EFT interactions Light Nuclei from Petr Navratil Lawrence Livermore National Laboratory* Collaborators: V. G. Gueorguiev (UCM), J. P. Vary (ISU), W. E. Ormand (LLNL), A. Nogga (Julich), S.

562 views • 42 slides
Part II: (S)RG and Low-Momentum Interactions To understand the properties of complex nuclei from

Part II: (S)RG and Low-Momentum Interactions To understand the properties of complex nuclei from

Part II: (S)RG and Low-Momentum Interactions To understand the properties of complex nuclei from first principles Renormalizing NN Interactions Basic ideas of RG Low-momentum interactions Similarity RG interactions Benefits of low cutoffs

862 views • 49 slides
Effective Field Theories for Electroweak Interactions in Nuclei Saori Pastore Winter Workshop on

Effective Field Theories for Electroweak Interactions in Nuclei Saori Pastore Winter Workshop on

Effective Field Theories for Electroweak Interactions in Nuclei Saori Pastore Winter Workshop on Neutrino-Nucleus Interactions FNAL - Batavia IL - November 2017 WITH nnn Schiavilla (ODU and JLab) & Carlson, Cirigliano, Dekens, Gandolfi,

837 views • 63 slides
Medium-mass nuclei from nuclear forces Achim Schwenk NUSTAR annual meeting, GSI, March 2, 2017

Medium-mass nuclei from nuclear forces Achim Schwenk NUSTAR annual meeting, GSI, March 2, 2017

Medium-mass nuclei from nuclear forces Achim Schwenk NUSTAR annual meeting, GSI, March 2, 2017 Nuclei bound by strong interactions ~ 3000 nuclei discovered (288 stable), 118 elements ~ 4000 nuclei unknown, extreme neutron-rich Nuclei bound by

757 views • 29 slides
Pe PeriScope: A : An E n Effect ectiv ive P e Probing bing and F and Fuz uzzing F ing

Pe PeriScope: A : An E n Effect ectiv ive P e Probing bing and F and Fuz uzzing F ing

Pe PeriScope: A : An E n Effect ectiv ive P e Probing bing and F and Fuz uzzing F ing Fram amework f k for t the he Har Hardwar are-OS B OS Boundar undary Dokyung Song, Felicitas Hetzelt, Dipanjan Das, Chad Spensky, Yeoul Na,

741 views • 27 slides
HARP collaboration results on the proton-nuclei interactions at a few GeV energies HARP : A

HARP collaboration results on the proton-nuclei interactions at a few GeV energies HARP : A

HARP collaboration results on the proton-nuclei interactions at a few GeV energies HARP : A fixed-target experiment at the CERN Proton Synchrotron (2000-2002) aimed at measurement of hadron production cross-sections for : Neutrino Factory

567 views • 53 slides
Investigation of the lowenergy kaons hadronic interactions in light nuclei by AMADEUS Dr.

Investigation of the lowenergy kaons hadronic interactions in light nuclei by AMADEUS Dr.

Investigation of the lowenergy kaons hadronic interactions in light nuclei by AMADEUS Dr. Kristian Piscicchia* Museo Storico della Fisica e Centro Studi e Ricerche Enrico Fermi INFN, Laboratori Nazionali di Frascati on behalf of the AMADEUS

1.41k views • 127 slides
The nuclear EMC effect in the deep-inelastic and the resonance region Sergey Kulagin Institute

The nuclear EMC effect in the deep-inelastic and the resonance region Sergey Kulagin Institute

The nuclear EMC effect in the deep-inelastic and the resonance region Sergey Kulagin Institute for Nuclear Research of the Russian Academy of Sciences, Moscow Talk at the XVth International Seminar on Electromagnetic Interactions of Nuclei

392 views • 37 slides
Generalized tensor methods and entanglement measurements for models with long-range interactions

Generalized tensor methods and entanglement measurements for models with long-range interactions

Generalized tensor methods and entanglement measurements for models with long-range interactions Ors Legeza in collaboration with Jen o S olyom, Gergely Barcza (Budapest) Florian Gebhard, Reinhard M. Noack (Marburg) Valentin

747 views • 64 slides
Atomic nuclei: from fundamental interactions to structure and stars Kai Hebeler Mainz, April 7,

Atomic nuclei: from fundamental interactions to structure and stars Kai Hebeler Mainz, April 7,

Atomic nuclei: from fundamental interactions to structure and stars Kai Hebeler Mainz, April 7, 2016 New Vistas in Low-Energy Precision Physics (LEPP) The theoretical nuclear landscape several years ago... Ab initio nuclear structure theory

735 views • 60 slides
Ab Initio Approaches to Light Nuclei Lecture 3: Light Nuclei Robert Roth Overview

Ab Initio Approaches to Light Nuclei Lecture 3: Light Nuclei Robert Roth Overview

Ab Initio Approaches to Light Nuclei Lecture 3: Light Nuclei Robert Roth Overview Lecture 1: Fundamentals Prelude Many-Body Quantum Mechanics Lecture 1: Nuclear Hamiltonian Nuclear Interactions Matrix Elements

506 views • 34 slides
Electromagnetic interactions of nuclei at the FCC-hh Igor Pshenichnov 1,*) , Sergey Gunin 1,2) 1)

Electromagnetic interactions of nuclei at the FCC-hh Igor Pshenichnov 1,*) , Sergey Gunin 1,2) 1)

Electromagnetic interactions of nuclei at the FCC-hh Igor Pshenichnov 1,*) , Sergey Gunin 1,2) 1) Institute for Nuclear Research, Russian Academy of Sciences, Moscow, Russia 2) Moscow Institute of Physics and Technology, Moscow Region, Russia *)

649 views • 44 slides
Probing Majorana modes using entanglement measures and fractional ac Josephson effect Moitri

Probing Majorana modes using entanglement measures and fractional ac Josephson effect Moitri

Probing Majorana modes using entanglement measures and fractional ac Josephson effect Moitri Maiti Bogoliubov Laboratory of Theoretical Physics (BLTP), Joint Institute for Nuclear Physics (JINR) Novel Quantum States in Condensed Matter 20th

638 views • 40 slides
Dark Matter Interactions with Nuclei Michael Wagman P.I. Phiala Shanahan Blue Waters Symposium

Dark Matter Interactions with Nuclei Michael Wagman P.I. Phiala Shanahan Blue Waters Symposium

Dark Matter Interactions with Nuclei Michael Wagman P.I. Phiala Shanahan Blue Waters Symposium 2019 What we know e e e Gravity Electromagnetism e Weak Force Strong Force e 2 What we know 3 <latexit

433 views • 20 slides
Efimov Effect in 2-Neutron Halo Nuclei Indranil Mazumdar Dept. of Nuclear & Atomic Physics,

Efimov Effect in 2-Neutron Halo Nuclei Indranil Mazumdar Dept. of Nuclear & Atomic Physics,

Efimov Effect in 2-Neutron Halo Nuclei Indranil Mazumdar Dept. of Nuclear & Atomic Physics, Tata Institute of Fundamental Research, Mumbai 400 005 Critical Stability Erice, 0ct.08 Halo World: The story according to Faddeev, Efimov and

686 views • 39 slides
Quantum Monte Carlo calculations for light nuclei using chiral forces Joel Lynn Theoretical

Quantum Monte Carlo calculations for light nuclei using chiral forces Joel Lynn Theoretical

Quantum Monte Carlo calculations for light nuclei using chiral forces Joel Lynn Theoretical Division, Los Alamos National Laboratory March 19, 2014 Outline 1 Motivation Ab-initio calculations for nuclei Nuclear interactions Phenomenology

703 views • 35 slides
Tensor For F , F Sh( X ) we have F F Sh( X ). Since tensor commutes with

Tensor For F , F Sh( X ) we have F F Sh( X ). Since tensor commutes with

Tensor For F , F Sh( X ) we have F F Sh( X ). Since tensor commutes with taking stalk, the non-exactness comes from that F x might not torsion-free, and this can be taken care by a simple resolution 0 P P F

1.85k views • 7 slides
Investigation of the low-energy kaons Investigation of the low-energy kaons hadronic interactions

Investigation of the low-energy kaons Investigation of the low-energy kaons hadronic interactions

Investigation of the low-energy kaons Investigation of the low-energy kaons hadronic interactions in light nuclei by hadronic interactions in light nuclei by AMADEUS AMADEUS K. Piscicchia* On behalf of the AMADEUS collaboration

977 views • 54 slides
Occultations for Probing for Probing Occultations Atmosphere and Climate: Atmosphere and

Occultations for Probing for Probing Occultations Atmosphere and Climate: Atmosphere and

I nstitute for G eophysics, A strophysics, and M eteorology / U niversity of G raz A tmospheric R emote S ensing and Cli mate Sys tem Research Group ARSCliSys on the art of understanding the climate system Occultations for Probing for Probing

570 views • 12 slides
8. Tensor Field Visualization Tensor: extension of concept of scalar and vector Tensor data

8. Tensor Field Visualization Tensor: extension of concept of scalar and vector Tensor data

8. Tensor Field Visualization Tensor: extension of concept of scalar and vector Tensor data for a tensor of level k is given by t i1,i2,,ik (x 1 ,,x n ) Second-order tensor often represented by matrix Examples:

292 views • 15 slides
Effect of aerosol-radiation and aerosol-cloud interactions in the simulation of photovoltaic and

Effect of aerosol-radiation and aerosol-cloud interactions in the simulation of photovoltaic and

Effect of aerosol-radiation and aerosol-cloud interactions in the simulation of photovoltaic and wind power using regional climate models Sonia Jerez*, Jose Mara Lpez-Romero, Blas Lajarin, Raquel Lorente-Plazas, Laura Palacios-Pea, Pedro

810 views • 16 slides
Interactions In the additive model, the effect of one factor is not affected by the level of the

Interactions In the additive model, the effect of one factor is not affected by the level of the

ST 380 Probability and Statistics for the Physical Sciences Interactions In the additive model, the effect of one factor is not affected by the level of the other. For instance, 1 , 1 2 , 1 = 1 2 = 1 , 2 2 , 2 =

343 views • 20 slides
Nuclear Matrix Elements for Tensor Interactions that Violate Local Lorentz Invariance Alex Brown

Nuclear Matrix Elements for Tensor Interactions that Violate Local Lorentz Invariance Alex Brown

Nuclear Matrix Elements for Tensor Interactions that Violate Local Lorentz Invariance Alex Brown and Vladimir Zelevinsky Alex Brown and Vladimir Zelevinsky National Superconducting Cyclotron Laboratory and Department of Physics and Astronomy

628 views • 35 slides
Isovector Dependence of the EMC Effect December 4, 2016 SRC/EMC 2016 IV EMC 1/9

Isovector Dependence of the EMC Effect December 4, 2016 SRC/EMC 2016 IV EMC 1/9

Isovector Dependence of the EMC Effect December 4, 2016 SRC/EMC 2016 IV EMC 1/9 Flavor-modifying EMC effect in asymmetric nuclei is not well constrained and would represent new information on medium modification Existance of flavor

561 views • 37 slides

More recommend