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Neutron Conversion Factors

Neutron Conversion Factors. E (meV) = 81.80 λ -2 (Å -2 ) E (meV) = 2.072 k 2 (Å -2 ) E (meV) = 5.227 × 10 6 τ -2 (m 2 / μ sec 2 ) T (K) = 11.604 E (meV). where τ is the time of flight, or inverse velocity ( τ = 1/v). E i , k i. φ. E f , k f. Inelastic Scattering Processes.

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Neutron Conversion Factors

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  1. Neutron Conversion Factors • E (meV) = 81.80 λ-2 (Å-2) • E (meV) = 2.072 k2 (Å-2) • E (meV) = 5.227 × 106τ-2(m2/μsec2) • T (K) = 11.604 E (meV) where τis the time of flight, or inverse velocity (τ= 1/v).

  2. Ei, ki φ Ef, kf Inelastic Scattering Processes Conservation of energy Conservation of “momentum”

  3. Reciprocal Space Construction The scattering triangle

  4. kf Q ki Ewald Spheres ki= 2π / λi kf= 2π / λf Q = ki- kf

  5. ψ ki -kf Q Kinematic Range From the scattering triangle, we can see that from which it follows that and so putting Ef =Ei - ε we get This equation gives us the locus of (Q, ε) for a given scattering angle ψ. (N.B. we can write ℏ2/2m=2.072 for E(meV) and Q in Å-1).

  6. ψ ki -kf Q Locus of Neutrons in (Q,ε) Space ε= Ei ψ = 118° Q→2ki ψ = 2.5°

  7. Scattering in ZrH2

  8. ki ψ Q⎜⎜ Q⊥ -kf Q Kinematics in a single crystal Can also be expressed in terms of the components of Q parallel and perpendicular to the incident wavevector ki: Hence it follows that and Q⊥ = kf sin (ψ) Q ⎜⎜ =ki – kf cos (ψ) This results in the surface of a paraboloid, with the apex in (Q//, Q⊥,ε)-space at the point (ki, 0, Ei).

  9. Kinematics in a Single Crystal (contd) In a single crystal experiment,we need to superimpose the scattering triangle on the reciprocal lattice. Locus of constant w is a Q-circle of radius kf centered on Q = ki ki [0,k,0] Q -kf [h,0,0]

  10. hω kI kF Q|| Q Q⊥ La0.7Pb0.3MnO3 - CMR Ferromagnet

  11. Specification: • 20meV< EI< 2000meV • lmod-chop = 10m • lsam-det = 6m • low angle bank: 3°-20° high angle bank: → 60° • Δhω/EI = 1- 5% (FWHH) • ~ 50% more flux • or ~ 25% better resln. • 40,000 detector elements • 2500 time channels • →108 pixels ≡ 0.4GBdatasets MAPS spectrometer Background chopper Monochromating chopper Sample position Position sensitive detector array cf SEQUOIA and ARCS at SNS

  12. Spin Waves in Cobalt H = -J ΣSi.Sj 12SJ = 199±7 meV γ = 69 ±12 meV

  13. k ⊥ c

  14. Stephen Nagler (ORNL) Bella Lake(Oxford) Alan Tennant (St. Andrews) Radu Coldea(ISIS/ORNL) KCuF3 Excitations (again) Direct observation of the continuum

  15. GUI interface run info. sample 2D & 1D cuts 2D slices in (Q,ω) 1D cuts in (Q,ω) Current Analysis Software MSLICE - Radu Coldea (ISIS/ORNL)

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