Difference between revisions of "R1n dnp.m"
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R1n=r1n_dnp(B0,T,g,T1e,T1n_bulk,r,bet) | R1n=r1n_dnp(B0,T,g,T1e,T1n_bulk,r,bet) | ||
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B0 - main magnet field, Tesla | B0 - main magnet field, Tesla | ||
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==See also== | ==See also== | ||
| − | [[Textbook module]] | + | [[brokensymm.m]], [[levelpop.m]], [[quad_shift.m]], [[r1csa2tauc.m]], [[r2csa2tauc.m]], [[rlx_csa.m]], [[rlx_dd_csa.m]], [[rlx_dip.m]], [[rlx_hfc.m]], [[rlx_nqi.m]], [[trosy_eff.m]], [[Textbook module]] |
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''Version 2.11, authors: [[Shebha Anandhi Jegadeesan]], [[Ilya Kuprov]], [[Guinevere Mathies]]'' | ''Version 2.11, authors: [[Shebha Anandhi Jegadeesan]], [[Ilya Kuprov]], [[Guinevere Mathies]]'' | ||
Latest revision as of 19:40, 6 June 2026
A simple model for nuclear longitudinal relaxation rate due to the presence of an unpaired electron in cryogenic DNP settings.
Syntax
R1n=r1n_dnp(B0,T,g,T1e,T1n_bulk,r,bet)
Parameters
B0 - main magnet field, Tesla T - absolute temperature, Kelvin g - electron g-factor, Bohr magneton units T1e - electron longitudinal relaxation time, seconds T1n_bulk - nuclear longitudinal relaxation time far away from the electron r - electron-nuclear distance, Angstrom bet - angle between the magnet field and the electron-nuclear direction, radians
Outputs
R1n - nuclear relaxation rate, Hz
See also
brokensymm.m, levelpop.m, quad_shift.m, r1csa2tauc.m, r2csa2tauc.m, rlx_csa.m, rlx_dd_csa.m, rlx_dip.m, rlx_hfc.m, rlx_nqi.m, trosy_eff.m, Textbook module
Version 2.11, authors: Shebha Anandhi Jegadeesan, Ilya Kuprov, Guinevere Mathies
