Neutron Compton Scattering as a Probe Of Hydrogen Bonded Systems - - PDF document

neutron compton scattering as a probe of hydrogen bonded
SMART_READER_LITE
LIVE PREVIEW

Neutron Compton Scattering as a Probe Of Hydrogen Bonded Systems - - PDF document

Neutron Compton Scattering as a Probe Of Hydrogen Bonded Systems George Reiter Jerry Mayers Collaborators P. Platzman J. Noreland J.C.Li Outline How do You Extract the Momentum Dis- tribution? How Much Detail Can One See? How Does


slide-1
SLIDE 1

Neutron Compton Scattering as a Probe Of Hydrogen Bonded Systems

George Reiter Jerry Mayers Collaborators

  • P. Platzman
  • J. Noreland

J.C.Li

slide-2
SLIDE 2

Outline

How do You Extract the Momentum Dis- tribution? How Much Detail Can One See? How Does Tunnelling Show Up? Results For KDP Results for Water and Ice

slide-3
SLIDE 3

Neutron Scattering in the Impulse Approximation Limit Deep Inelastic Neutron Scattering

SM( q, ω) =

n(

p)δ(ω − ¯

hq2 2M − p. q M )d

p ¯ hω is the energy transfer, M is the mass of the tar- get particle, q=| q| is the magnitude of the wavector transfer and n( p) is the momentum distribution. SM( q, ω) = M

q

n(

p)δ(y − p.ˆ q)d p = M

q J(ˆ

q, y) y=M

q (ω − ¯ hq2 2M ), ˆ

q= q/q

slide-4
SLIDE 4

A Very Useful Theorem

If we express J(ˆ q, y) as

J(ˆ q, y) = e−y2

π

1 2

  • n,l,m

an,l,mH2n+l(y)Ylm(ˆ q)

then

n( p) = e−p2

π

3 2

  • n,l,m

22n+ln!(−1)nan,l,mplL

l+1

2

n

(p2)Ylm(ˆ p)

slide-5
SLIDE 5

Statistical Errors in Measured n( p)

δn( p) =

  • i

δn( p) δρi δρi

< δn( p)2 >=

  • i,j

δn( p) δρi δn( p) δρj

< δρiδρj >

slide-6
SLIDE 6

5 10 15 20 25

pz-inv. Angstroms

0.001 0.002 0.003 0.004 0.005 0.006 0.007

n(p)

momentum distribution error limits anharmonicity

Momentum Distribution Along Bond

slide-7
SLIDE 7

KHC2O4

slide-8
SLIDE 8

Momentum Distribution for Two Displaced Gaussians

  • f Relative Weight r

n(px, py, pz)=(1+r2+2rcos(2pza))

(1+r2+2re

− a2 2σz2)

  • i

e

− p2 i 2σ2 i

(2πσi)

1 2

If r=1,then n(px, py, pz)=2cos2(pza)

(1+e

−a2 2σz2)

  • i

e

− p2 i 2σ2 i

(2πσi)

1 2

slide-9
SLIDE 9
slide-10
SLIDE 10

−0.002 0.002 0.004 0.006 0.008

n(p)

10 20 30 Momentum (Inv. Angstroms)

KDP Momentum Distribution Along Bond

T=130K T=90K 10 20 30 Ab−initio Experiment

slide-11
SLIDE 11

Direct Measurement of the Born-Oppenheimer Potential Φ( p) = ±

  • n(

p) Ψ( r) =

ei

p· rΦ(

p)d p E − V ( r) =

p2

2Mei p· rΦ(

p)d p

ei

p· rΦ(

p)d p

slide-12
SLIDE 12

−0.4 −0.3 −0.2 −0.1 0.1 0.2 0.3 0.4 Angstroms −500 500 1000 1500 2000 MILLI−EV

KDP Potential and Wavefunction

Potential Wave Function(arb. units)

slide-13
SLIDE 13
slide-14
SLIDE 14

10 20 30 momentum−inv. angstroms 0.002 0.004 0.006 0.008 0.01 radial momentum distribution p**2 n(p)

hydrogen momentum distribution in water

ice −4C 23C 1bar 300C 100 bar 400C 750 bar errors errors

slide-15
SLIDE 15

Simulated Data, r=.5