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Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department of Physics, University of Warwick

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Page 1: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Electron nuclear double resonance (ENDOR)

Gavin W Morley,

Department of Physics,

University of Warwick

Page 2: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Electron nuclear double resonance (ENDOR)

Overview-Why do ENDOR?-Continuous-wave ENDOR-Pulsed ENDOR with:

- Selective pulses- Non-selective pulses

Page 3: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Electron nuclear double resonance (ENDOR)

-Why do ENDOR?

- More sensitive than NMR - “EPR-detected NMR” (electron has a

larger magnetic moment, flips faster and can be detected more sensitively)

- NMR may be impossible due to nearby electron spin

- Higher resolution than EPR- Extra selection rules

Page 4: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

George Feher (born 1924) Photo from AIP Emilio Segre Visual Archives

Image by Manuel Vögtli (UCL)

Birth of ENDOR

Page 5: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

EPR-detected NMR: how?

Electron nuclear double resonance (ENDOR)

Page 6: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Energy of a spin system

Magnetic field, B

Photons reflected

S = ½ I = ½

Iz = ½ Iz = -½

Magnetic field, B

Electron paramagnetic resonance

Page 7: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Energy of a spin system

Magnetic field, B

Photons reflected

Iz = ½ Iz = -½

Magnetic field, B

Electron paramagnetic resonance

S = ½ I = ½

You need to record an EPR spectrum before trying ENDOR

Page 8: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Energy of a spin system

Magnetic field, B

Photons reflected

Iz = ½ Iz = -½

Magnetic field, B

ENDOR

RF in

S = ½ I = ½

Page 9: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Microwave photons reflected

RF frequency

Two ENDOR transition frequencies

For isotropic A

“Weak coupling”

Microwave photons reflected

RF frequency

“Strong coupling”

Page 10: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Energy of a spin system

Magnetic field, B

Photons reflected

Iz = ½ Iz = -½

Electron paramagnetic resonance

Magnetic field, B

Page 11: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Energy of a spin system

Magnetic field, B

Electron paramagnetic resonance

Page 12: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

B0 is static magnetic fieldB1 is EPR magnetic fieldB2 is NMR magnetic field

• EPR-detected NMR: how?

Electron nuclear double resonance (ENDOR)

Page 13: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

B0 is static magnetic fieldB1 is EPR magnetic fieldB2 is NMR magnetic field

• EPR-detected NMR: how?

Electron nuclear double resonance (ENDOR)

Page 14: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

B0 is static magnetic fieldB1 is EPR magnetic fieldB2 is NMR magnetic field

• EPR-detected NMR: how?

Electron nuclear double resonance (ENDOR)

Page 15: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

B0 is static magnetic fieldB1 is EPR magnetic fieldB2 is NMR magnetic field

• EPR-detected NMR: how?

Electron nuclear double resonance (ENDOR)

Page 16: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

EPR-detected NMR

Continuous Wave ENDOR

George Feher Photo from AIP Emilio Segre Visual Archives

Image by Manuel Vögtli (UCL)

Page 17: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Continuous Wave ENDOR

Page 18: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Continuous Wave ENDOR

Page 19: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Continuous Wave ENDOR

CW ENDOR is the desaturation of a saturated EPR transition by providing an extra T1e relaxation route via NMR

Page 20: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Continuous Wave ENDOR

Hale & Mieher, Phys Rev 184 739 (1969)(following Feher, Phys Rev 114, 1219 (1959))

νNMR (MHz)

CW ENDOR is the desaturation of a saturated EPR transition by providing an extra T1e relaxation route via NMR

(use FM and lock-in)

Page 21: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Continuous Wave ENDOR

νNMR (MHz)

Image by Manuel Vögtli (UCL)

B Koiller, R B Capaz, X Hu and S Das Sarma, PRB 70, 115207 (2004)

Hale & Mieher, Phys Rev 184 739 (1969)(following Feher, Phys Rev 114, 1219 (1959))

Page 22: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Continuous Wave ENDOR

νNMR (MHz)

CW ENDOR effect is typically a few % of the EPR signal

Hale & Mieher, Phys Rev 184 739 (1969)(following Feher, Phys Rev 114, 1219 (1959))

Page 23: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Continuous Wave ENDOR

George Feher Photo from UCSD

Advantage of CW ENDOR: Observe sharpest ENDOR resonances

Disadvantage of CW ENDOR: CW ENDOR line intensity depends on a delicate balance between relaxation rate and excitation power. Jack Freed did the relaxation theory for this for molecules in solution.

This is compared with experiments in solution in:Plato, Lubitz & Mobius, J Phys Chem 85, 1202 (1981)

Page 24: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Pulsed ENDOR

Use a π pulse for nuclei, but there are two main pulse sequences for electrons:

1.Davies ENDOR: π pulse then echo readout with all selective (long) pulses.

2.Mims ENDOR uses a stimulated echo with non-selective (short) pulses

Page 25: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Roy Davies, Royal Holloway, University of London

π

π π/2

RF:

MW:

As with CW ENDOR, sweep RF frequency to get a spectrum.

Use long, selective MW pulses to burn a hole smaller signal. However, there are no “blind spots” which is an advantage over Mims ENDOR.

π

Page 26: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Rotating frame

Page 27: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Rotating frame

Page 28: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Spin echo

In rotating frame

Page 29: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Spin echo

In rotating frame

Page 30: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Product operator notation:Electron-nuclear two-spin order, 2SzIz

Page 31: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

RF pulse duration is an important parameter to set

Page 32: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Echo height

RF frequency

Davies ENDOR efficiency, FDavies= 50%

Page 33: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Product operator notation:Electron-nuclear two-spin order, 2SzIz

Start again…

Page 34: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Off-resonance RF does nothing

Page 35: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Echo height

RF frequency

Page 36: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Product operator notation:Electron-nuclear two-spin order, 2SzIz

Start again again…

Page 37: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Page 38: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Echo height

RF frequency

Davies ENDOR efficiency, FDavies= 50%

Page 39: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Davies ENDOR

Davies ENDOR disadvantage: selective pulses on electron spins mean many spins are ignored if the resonance is inhomogeneously broadened

Page 40: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Mims ENDOR

τ τπ

RF: sweep RF frequency

MW:

Non-selective (short) MW pulses excite more spins bigger signal.

However, ENDOR efficiency, FMims = ¼ (1 – cos (A τ))

so there are “blind spots” with no signal for some τ

Page 41: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Mims ENDOR

Page 42: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Beware Mims ENDOR blind spots

ENDOR efficiency,

FMims = ¼ (1 – cos (A τ))

C Gemperle & A Schweiger, Chem Rev 91, 1481 (1991)

Page 43: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Beware short RF pulses in pulsed ENDOR

C Gemperle & A Schweiger, Chem Rev 91, 1481 (1991)

This problem is avoided by “time-domain pulsed ENDOR”, instead of the standard frequency domain experiments.

Page 44: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

Pulsed ENDOR

For more details including TRIPLE (ENDOR with two RF frequencies) see:

Schweiger & Jeschke, Principles of pulse electron paramagnetic resonance, OUP 2001

C Gemperle & A Schweiger, Chem Rev 91, 1481 (1991)

Page 45: Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013 Electron nuclear double resonance (ENDOR) Gavin W Morley, Department

Introduction to ENDOR, Gavin W Morley, iMR CDT Advanced Workshop, 10 th April 2013

ENDOR conclusions

- ENDOR is much more sensitive than NMR and has much higher resolution than EPR

- Continuous-wave ENDOR for very sharp resonances

- Pulsed ENDOR with:- Selective pulses (Davies)- Non-selective pulses (Mims)