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Highlights of Core R & D at ACERT |
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Recent Highlights
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Scanned-probe detection of electron spin resonance from a nitroxide spin probe
We have developed an approach that extends the applicability of ultrasensitive force gradient detection of
magnetic resonance to samples with spin-lattice relaxation times (T1) as short as a single cantilever period. To demonstrate
the generality of the approach, which relies on detecting either cantilever frequency or phase, we used it to detect electron spin resonance
from a T1 = 1 ms nitroxide spin probe (cf. Figure) in a thin film at 4.2 K and 0.6 T. Using a custom fabricated cantilever
with a 4 μm diameter nickel tip, we achieve a magnetic resonance sensitivity of 410 Bohr magnetons in a 1 Hz bandwidth. Our theory for this
quantitatively predicts both the lineshape and the magnitude of the observed cantilever frequency shift as a function of field and
cantilever-sample separation. Good agreement was found between nitroxide T1’s measured mechanically and inductively,
indicating that the cantilever magnet is not an appreciable source of spin-lattice relaxation here. We suggest that the new approach has a number
of advantages that make it well suited to push magnetic resonance detection and imaging of nitroxide spin labels in an individual macromolecule
to single-spin sensitivity. In the figure below, we show the schematic of the scanned-probe electron spin resonance experiment. A
microstripline half-wave resonator delivers a transverse magnetic field, B1, oscillating at 17.7 GHz. In the center of the resonator,
the microwave field oscillates along the x direction. A longitudinal Zeeman field of magnitude B0 ˜ 0:6 T is applied along the z
axis. The high-compliance cantilever has its long axis along y and oscillates in the x direction. The cantilever’s 4 μm-diameter nickel tip
was affixed by hand. The sample is a 230 nm-thick film of 40 mM TEMPAMINE in perdeuterated polystyrene, coated with 20 nm of gold. The sample
film was spin-coated onto a 250 μm-thick quartz wafer. For clarity, sample and substrate are not drawn to scale.
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Eric W. Moore, Sang Gap Lee, Steven A. Hickman, Sarah J. Wright, (Dept. of Chemistry and Chemical Biology, Cornell University, Ithaca, NY
14853)
Lee E. Harrell, (Dept. of Physics, U.S. Military Academy, West Point, NY 10996)
Peter P. Borbat, Jack H. Freed, and John A. Marohn (Dept. of Chemistry and Chemical Biology, Cornell University, Ithaca, NY 14853)
July 2009
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