The main limitation of pulse electron paramagnetic resonance (EPR) spectroscopy is its narrow excitation bandwidth. Ultra-wideband (UWB) excitation with frequency-swept chirp pulses over several hundreds of megahertz overcomes this drawback. This allows to excite electron spin echo envelope modulation (ESEEM) from paramagnetic copper centers in crystals, whereas up to now, only ESEEM of ligand nuclei like protons or nitrogens at lower frequencies could be detected. ESEEM spectra are recorded as two-dimensional correlation experiments, since the full digitization of the electron spin echo provides an additional Fourier transform EPR dimension. Thus, UWB hyperfine-sublevel correlation experiments generate a novel three-dimensional EPR-correlated nuclear modulation spectrum.

1.
A.
Schweiger
and
G.
Jeschke
,
Principles of Pulse Electron Paramagnetic Resonance
(
Oxford University Press
,
2001
).
2.
R. R.
Ernst
,
G.
Bodenhausen
, and
A.
Wokaun
,
Principles of Nuclear Magnetic Resonance in One and Two Dimensions
(
Clarendon Press
,
1990
).
3.
P.
Höfer
,
A.
Grupp
,
H.
Nebenführ
, and
M.
Mehring
, “
Hyperfine sublevel correlation (HYSCORE) spectroscopy: A 2D ESR investigation of the squaric acid radical
,”
Chem. Phys. Lett.
132
,
279
282
(
1986
).
4.
L. G.
Rowan
,
E. L.
Hahn
, and
W. B.
Mims
, “
Electron-spin-echo envelope modulation
,”
Phys. Rev.
137
,
A61
A71
(
1965
).
5.
W. B.
Mims
, “
Envelope modulation in spin-echo experiments
,”
Phys. Rev. B
5
,
2409
2419
(
1972
).
6.
Y.
Deligiannakis
,
M.
Louloudi
, and
N.
Hadjiliadis
, “
Electron spin echo envelope modulation (ESEEM) spectroscopy as a tool to investigate the coordination environment of metal centers
,”
Coord. Chem. Rev.
204
,
1
112
(
2000
).
7.
G.
Jeschke
and
A.
Schweiger
, “
Time-domain chirp electron nuclear double resonance spectroscopy in one and two dimensions
,”
J. Chem. Phys.
103
,
8329
8337
(
1995
).
8.
L. V.
Kulik
,
B.
Epel
,
W.
Lubitz
, and
J.
Messinger
, “
Electronic structure of the Mn4OxCa cluster in the S0 and S2 states of the oxygen-evolving complex of photosystem II based on pulse 55Mn-ENDOR and EPR spectroscopy
,”
J. Am. Chem. Soc.
129
,
13421
13435
(
2007
).
9.
A.
Doll
and
G.
Jeschke
, “
Fourier-transform electron spin resonance with bandwidth-compensated chirp pulses
,”
J. Magn. Reson.
246
,
18
26
(
2014
).
10.
G.
Jeschke
,
S.
Pribitzer
, and
A.
Doll
, “
Coherence transfer by passage pulses in electron paramagnetic resonance spectroscopy
,”
J. Phys. Chem. B
(in press).
11.
G.
Jeschke
, “
DEER distance measurements on proteins
,”
Annu. Rev. Phys. Chem.
63
,
419
446
(
2012
).
12.
A.
Doll
,
S.
Pribitzer
,
R.
Tschaggelar
, and
G.
Jeschke
, “
Adiabatic and fast passage ultra-wideband inversion in pulsed EPR
,”
J. Magn. Reson.
230
,
27
39
(
2013
).
13.
P. E.
Spindler
,
S. J.
Glaser
,
T. E.
Skinner
, and
T. F.
Prisner
, “
Broadband inversion PELDOR spectroscopy with partially adiabatic shaped pulses
,”
Angew. Chem., Int. Ed.
52
,
3425
3429
(
2013
).
14.
A.
Doll
,
M.
Qi
,
S.
Pribitzer
,
N.
Wili
,
M.
Yulikov
,
A.
Godt
, and
G.
Jeschke
, “
Sensitivity enhancement by population transfer in Gd(III) spin labels
,”
Phys. Chem. Chem. Phys.
17
,
7334
7344
(
2015
).
15.
P.
Schöps
,
P. E.
Spindler
,
A.
Marko
, and
T. F.
Prisner
, “
Broadband spin echoes and broadband SIFTER in EPR
,”
J. Magn. Reson.
250
,
55
62
(
2015
).
16.
J.
Gorcester
and
J. H.
Freed
, “
Two-dimensional Fourier transform ESR spectroscopy
,”
J. Chem. Phys.
85
,
5375
5377
(
1986
).
17.
H. M.
McConnell
,
C.
Heller
,
T.
Cole
, and
R. W.
Fessenden
, “
Radiation damage in organic crystals. I. CH(COOH)2 in malonic acid
,”
J. Am. Chem. Soc.
82
,
766
775
(
1960
).
18.
S.
Lee
,
B. R.
Patyal
, and
J. H.
Freed
, “
A two-dimensional Fourier transform electron-spin resonance (ESR) study of nuclear modulation and spin relaxation in irradiated malonic acid
,”
J. Chem. Phys.
98
,
3665
3689
(
1993
).
19.
K.
Nagayama
,
K.
Wüthrich
, and
R. R.
Ernst
, “
Two-dimensional spin echo correlated spectroscopy (SECSY) for 1H NMR studies of biological macromolecules
,”
Biochem. Biophys. Res. Commun.
90
,
305
311
(
1979
).
20.
J.-M.
Böhlen
,
M.
Rey
, and
G.
Bodenhausen
, “
Refocusing with chirped pulses for broadband excitation without phase dispersion
,”
J. Magn. Reson.
84
,
191
197
(
1989
).
21.
J.
Baum
,
R.
Tycko
, and
A.
Pines
, “
Broadband and adiabatic inversion of a two-level system by phase-modulated pulses
,”
Phys. Rev. A
32
,
3435
3447
(
1985
).
22.
See supplementary material at http://dx.doi.org/10.1063/1.4927088 for futher experimental and simulated 2D EPR/ESEEM spectra and the resonator profile.
23.
A. T.
Brant
,
S.
Yang
,
N. C.
Giles
,
M.
Zafar Iqbal
,
A.
Manivannan
, and
L. E.
Halliburton
, “
Oxygen vacancies adjacent to Cu2+ ions in TiO2 (rutile) crystals
,”
J. Appl. Phys.
109
,
073711
(
2011
).
24.
E. S.
Sabisky
and
H. J.
Gerritsen
, “
Measurements of dielectric constant of rutile (TiO2) at microwave frequencies between 4.2 and 300K
,”
J. Appl. Phys.
33
,
1450
1453
(
1962
).
25.
J. A.
Ferretti
and
R. R.
Ernst
, “
Interference effects in NMR correlation spectroscopy of coupled spin systems
,”
J. Chem. Phys.
65
,
4283
4293
(
1976
).
26.
A.
Ponti
and
A.
Schweiger
, “
Nuclear coherence-transfer echoes in pulsed EPR
,”
J. Chem. Phys.
102
,
5207
5219
(
1995
).
27.
J.
Ammeter
,
G.
Rist
, and
Hs. H.
Günthard
, “
Influence of the host lattice upon EPR coupling parameters and d-d transitions of planar copper (II) complexes
,”
J. Chem. Phys.
57
,
3852
3866
(
1972
).

Supplementary Material

You do not currently have access to this content.