Coherent electron spin manipulation in a dilute oriented ensemble of molecular nanomagnets: pulsed EPR on doped single crystals†

The study of coherent electron spin dynamics in molecular nanomagnets (MNMs) has recently become the subject of intense research. This is inspired in part by proposals for quantum information processing, exploiting, for example, the large total spins and molecular size, intra-molecular excitations, and the ability to make more complex structures via supramolecular approaches. It is also important generally in the study of how such molecules interact with their environment. Pulsed EPR allows direct measurement of spin coherence; the first such studies for MNMs, on Cr7M heterometallic rings, revealed phase memory times (TM; quantifying the rate of loss of quantum phase information to the environment) of the order of ms at a few kelvin. This and subsequent studies were performed on dilute solutions, or doped into nanoporous silicon, in order to minimise decoherence due to intermolecular dipolar interactions. However, the sample is then an ensemble of randomly oriented molecules. Various proposals for MNMs depend on coherent manipulation of an anisotropic spin multiplet. Since transition energies depend on orientation, the lack of alignment limits the range of quantum information experiments that may be performed. The obvious way to address aligned samples is in single crystals. This requires alternative strategies to overcome inter-molecular driven decoherence. Takahashi et al. reported pulsed 240 GHz EPR on crystals of Fe8 under very high magnetic fields that quench electron spin flip-flop relaxation. The alternative is to dilute the MNM in an isostructural and diamagnetic host. This is straightforward for monometallic complexes, but for high nuclearity d-block clusters it is rarely possible to prepare the diamagnetic equivalent. Here we present single-crystal pulsed X-band EPR studies on (Me2NH2)[Cr7ZnF8(O2C Bu)16] (Cr7Zn), achieved by doping into the diamagnetic Ga7Zn analogue. Cr7Zn and Ga7Zn were prepared by adaptations of methods for other M7M (ESI†). 12 The metal ions in each molecule define a planar octagon, with each edge bridged by a fluoride and two pivalates, giving a complex anion which is centred on a Me2NH2 + cation (Fig. S1, ESI†). Single crystals of Cr7Zn (0.3% by mass) doped in Ga7Zn (Cr7Zn@ Ga7Zn), isostructural with the parent compounds, were grown from toluene. CW EPR (Fig. S2, ESI†) shows the Cr7Zn dopant is incorporated without scrambling of Cr and Ga. Cr7Zn has a well defined total spin S = 3/2 ground state, as characterised by INS and CW EPR, because the hetero-ion prevents complete cancellation of spin despite the antiferromagnetic coupling. At 5 K over 90% of the population (>99% at 2 K) is in the ground state, which therefore dominates the EPR, with the remainder in the S = 1/2 and 5/2 lowest excited states which lie at 6.7 and 15 cm , respectively, in zero-field. The ground state has axial and rhombic zero-field splitting (ZFS) parameters of D = 0.4186 and E = 0.0489 cm , respectively [spin Hamiltonian (1) with giso = 1.96; B is the applied magnetic field]. The ZFS is largely dominated by the single ions, but with important contributions from anisotropic exchange. The principal direction of the D tensor (the molecular z axis) is normal to the Cr7Zn plane (the xy plane). Ĥs = mBBgŜ + D[Ŝz 2 S(S + 1)/3] + E(Ŝx Ŝy) (1) Cr7Zn@Ga7Zn crystallises in the tetragonal I4 space group (ESI†), with the molecules lying on the C4 axis such that the M7Zn rings are in the crystal ab plane (Fig. 1). Crystals can be conveniently mounted (Fig. S3, ESI†) to allow EPR measurement in the bc plane (Fig. 2). The b and c axes (which we define as y = 90 and 01, respectively) are readily identified from the turning points in the resonance field road map (Fig. S4, ESI†). The coplanarity of the rings in the unit cell means there is only one magnetically distinct molecule when B is parallel to c (hence the molecular z axis). However, because the Zn ion is disordered over all sites of the Cr7Zn octagon, when B is off the c axis there are magnetically distinct molecules: if j is the projection of B onto the molecular xy plane then these correspond to j, j + 451, j + 901 and a School of Chemistry and Photon Science Institute, The University of Manchester, Oxford Road, Manchester M13 9PL, UK. E-mail: eric.mcinnes@manchester.ac.uk; Fax: +44 (0)161-275-1001; Tel: +44 (0)161-275-4469 b CAESR, The Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, UK. E-mail: a.ardavan1@physics.ox.ac.uk; Tel: +44 (0)1865 272366 † Electronic supplementary information (ESI) available: Syntheses; unit cell details; EPR spectra, crystal mounting, relaxation and nutation data. CCDC 954609 and 954610. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c3cc46326e Received 17th August 2013, Accepted 29th October 2013

clusters it is rarely possible to prepare the diamagnetic equivalent.
Cr 7 Zn and Ga 7 Zn were prepared by adaptations of methods for other M 0 7 M (ESI †). 12 The metal ions in each molecule define a planar octagon, with each edge bridged by a fluoride and two pivalates, giving a complex anion which is centred on a Me 2 NH 2 + cation (Fig. S1, ESI †).
Single crystals of Cr 7 Zn (0.3% by mass) doped in Ga 7 Zn (Cr 7 Zn@ Ga 7 Zn), isostructural with the parent compounds, were grown from toluene.CW EPR (Fig. S2, ESI †) shows the Cr 7 Zn dopant is incorporated without scrambling of Cr III and Ga III .Cr 7 Zn has a well defined total spin S = 3/2 ground state, as characterised by INS 13 and CW EPR, 14 because the hetero-ion prevents complete cancellation of spin despite the antiferromagnetic coupling.At 5 K over 90% of the population (>99% at 2 K) is in the ground state, which therefore dominates the EPR, with the remainder in the S = 1/2 and 5/2 lowest excited states which lie at 6.7 and 15 cm À1 , respectively, in zero-field. 14The ground state has axial and rhombic zero-field splitting (ZFS) parameters of D = À0.4186 and E = À0.0489cm À1 , respectively [spin Hamiltonian (1) with g iso = 1.96;B is the applied magnetic field].The ZFS is largely dominated by the single ions, but with important contributions from anisotropic exchange. 14The principal direction of the D tensor (the molecular z axis) is normal to the Cr 7 Zn plane (the xy plane).
Cr 7 Zn@Ga 7 Zn crystallises in the tetragonal I4 space group (ESI †), with the molecules lying on the C 4 axis such that the M 0 7 Zn rings are in the crystal ab plane (Fig. 1).Crystals can be conveniently mounted (Fig. S3, ESI †) to allow EPR measurement in the bc plane (Fig. 2).The b and c axes (which we define as y = 90 and 01, respectively) are readily identified from the turning points in the resonance field road map (Fig. S4, ESI †).The coplanarity of the rings in the unit cell means there is only one magnetically distinct molecule when B is parallel to c (hence the molecular z axis).However, because the Zn ion is disordered over all sites of the Cr 7 Zn octagon, when B is off the c axis there are magnetically distinct molecules: if j is the projection of B onto the molecular xy plane then these correspond to j, j + 451, j + 901 and a School of Chemistry and Photon Science Institute, The University of Manchester, Oxford Road, Manchester M13 9PL, UK.E-mail: eric.mcinnes@manchester.ac.uk;Fax: +44 (0)161-275-1001; Tel: +44 (0)161-275-4469 b CAESR, The Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, UK.E-mail: a.ardavan1@physics.ox.ac.uk;Tel: +44 (0)1865 272366 † Electronic supplementary information (ESI) available: Syntheses; unit cell details; EPR spectra, crystal mounting, relaxation and nutation data.CCDC 954609 and 954610.For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c3cc46326e j + 1351 (further rotations about c are equivalent).Hence we should observe four sets of resonances from distinct molecules in the bc plane, collapsing to one set at c.We have calculated 16 the single orientation spectra with this model, using the S = 3/2 parameters above; i.e. with no free variables other than a molecular azimuthal angle j which defines all four magnetically distinct molecules by symmetry.Good agreement is found for j = 161 (Fig. 2 and Fig. S4, ESI †).The simulations use a natural linewidth of 4 mT with a D-strain of 15% and a crystal mosaicity 15 of ca.2%.
The splitting of the spectrum into four inequivalent sites is most clearly resolved in the low-field transitions (Fig. 2), which have much narrower linewidths.This latter phenomenon is a result of the states involved in the transitions, as shown by calculated Zeeman diagrams for the S = 3/2 multiplet with B orientated just off the c axis and along b (Fig. 3).The low-field transitions are within a single Kramers doublet, while the high-field transitions are between the mixed |AE1/2i and |AE3/2i doublets.Hence, the former transitions are independent of the ZFS and are unaffected by D-strain. 14In contrast the latter transitions are significantly broadened by strain effects.
The doping reduces intermolecular effects sufficiently to allow single crystal pulsed EPR: we observe spin echoes with a standard Hahn sequence (p/2-t-p-t-echo) at temperatures below ca. 8 K. Xband field-swept echo-detected (FSED) spectra were measured on a polycrystalline sample (Fig. S5, ESI †) and on a single crystal at y = 0 and 901 (Fig. 3 and Fig. S5, ESI †) by integration of the echo intensity at various static applied fields (16 ns p/2 pulse with fixed delay t = 200 ns).There is a clear correspondence of the S = 3/2 ground state resonances between the CW and FSED spectra.
T M was measured for the 366, 545 and 1220 mT transitions at cJB by monitoring the decay of the echo intensity as a function of t and fitting to a stretched exponential function (Fig. S6, ESI †; ESEEM modulations due to 1 H are observed).T M increases gradually from 5 to 2.1 K, reaching 0.87, 0.66 and 0.58 AE 0.01 ms respectively (Fig. S7, ESI †).It should be possible to significantly enhance these values by: (i) further dilution.A 0.3% dopant level gives a statistical range of inter-spin separations and consequent dipolar interactions centred round ca.500 kHz.This frequency would put an upper limit of ca. 2 ms on the spin-spin relaxation time T 2 , comparable with our T M ; (ii) per-deuteration, reducing dipolar interactions with nuclear spins; 1 (iii) using carboxylates and cation without methyl groups, reducing spectral diffusion effects due to Me rotations and librations.We have previously achieved ca.ten-fold enhancements of T M for Cr 7 Ni in dilute solution by these methods. 6The T M values observed here are similar to those measured for Cr 7 Ni with the same ligand set; 6 this has an S = 1/2 ground state hence phonon driven modulation of the ZFS does not appear to be a dominant relaxation mechanism.T M values measured for bJB at 4.5 K are in the range of those measured for cJB (0.56 and 0.45 ms for B 0 = 612 and 840 mT), consistent with observations on Cr 7 Mn (S = 1) in frozen solution that T M varies little at different points (orientations) in the spectrum. 1inally we show that we can perform coherent spin manipulations on the Cr 7 Zn@Ga 7 Zn single crystal by nutation experiments.In this experiment, a nutation pulse of duration t p tips the   magnetisation through an angle gm B B 1 t p / h, followed by a two-pulse detection sequence [t p -T-p/2-t-p-t-echo, with fixed T and 4-step phase cycling].The echo intensity, quantifying the z-component of the magnetisation after the nutation pulse, is measured as function of t p .This experiment sets up a coherent oscillation between the two states, corresponding to generation of arbitrary superpositions, observed as oscillation of the echo intensity as a function of t p .Some authors describe these as Rabi oscillations, although this is only strictly correct when the pulse bandwidth substantially exceeds the EPR linewidth such that all spin packets rotate together.
We selected the highest-field and most isolated transition for cJB, with B 0 = 1160 mT, corresponding to the nominally m s = +1/2 to +3/2 transition with frequency 9.77 GHz.We find oscillations in the echo amplitude as a function of t p (Fig. 4; T = 256 ns and the p/2and p-pulses are optimised for the power).The oscillation frequency is proportional to the square root of microwave power (i.e. to the amplitude of the microwave field B 1 ; Fig. S8, ESI †), demonstrating that we are observing coherent electron spin oscillations rather than other phenomena such as ESEEM.The excitation bandwidth in this experiment is narrow compared to the inhomogeneous broadening of the line, leading to a nutation envelope that depends on oscillation number rather than time.
It has been noted in previous nutation experiments on MNMs in frozen solutions 2-4 that the distribution in molecular orientations being excited (each with a different nutation frequency) contributes to premature damping of the oscillations before the limits placed by T M .We have removed this factor in this single crystal experiment and the limiting factors may include D-strain and/or crystal mosaicity, with analogous effects.
In conclusion, we have reported the first pulsed EPR on single crystals of doped MNMs.This opens the way for coherent multifrequency experiments manipulating the quantum spin state, thereby testing proposals for their application in quantum information processing.This work highlights the utility of the M 0 7 M family in testing new theories and experiments for MNMs, due to their tuneable composition and magnetic properties. 16In this case, doping without scrambling of the metal ions is aided by the kinetic inertness of the Cr(III) ion.However, the fact that an Fe 4 -doped Ga 4 material has been synthesised (though pulsed EPR on it was not reported), 17 indicates that it is possible with more labile metal ions.Future targets will also include doped dimers of S = 1/2 ground state MNMs, which we can prepare with tuneable interaction strengths, 18 for potential use in logic gates in analogy to the organic-based chemistry of Takui and co-workers on doped single crystals of nitroxyl dimers. 19e are grateful to the EPSRC for funding, including for the National EPR Facility at Manchester and the Oxford CAESR.REPW thanks the Royal Society for a Wolfson Merit Award.

Fig. 2
Fig. 2 Single crystal CW X-band EPR of Cr 7 Zn@Ga 7 Zn in the bc plane at 5 K: experimental (thick) and simulated spectra (thin; summation over four molecular orientations, see text).Crystal orientations from y = 0 (top) to 901 (bottom); high-field regions Â20 for clarity.[The sharp feature at g = 1.96 (342 mT) is due to the S = 1/2 excited state.]

Fig. 3
Fig. 3 Top: Zeeman diagrams for the S = 3/2 ground state and X-band EPR transitions calculated for y = 81 (left) and 901 (right; different colours represent the four molecular orientations, see text).Bottom: experimental (black) and simulated (red) CW, and FSED (grey) spectra at 5 K. [The peak at 330 mT, marked *, is intrinsic to the resonator.]