School of Physics - Research Publications

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    Tuning Single Quantum Dot Emission with a Micromirror
    Yuan, G ; Gomez, D ; Kirkwood, N ; Mulvaney, P (AMER CHEMICAL SOC, 2018-02)
    The photoluminescence of single quantum dots fluctuates between bright (on) and dark (off) states, also termed fluorescence intermittency or blinking. This blinking limits the performance of quantum dot-based devices such as light-emitting diodes and solar cells. However, the origins of the blinking remain unresolved. Here, we use a movable gold micromirror to determine both the quantum yield of the bright state and the orientation of the excited state dipole of single quantum dots. We observe that the quantum yield of the bright state is close to unity for these single QDs. Furthermore, we also study the effect of a micromirror on blinking, and then evaluate excitation efficiency, biexciton quantum yield, and detection efficiency. The mirror does not modify the off-time statistics, but it does change the density of optical states available to the quantum dot and hence the on times. The duration of the on times can be lengthened due to an increase in the radiative recombination rate.
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    The Degradation and Blinking of Single CsPbl3 Perovskite Quantum Dots
    Yuan, G ; Ritchie, C ; Ritter, M ; Murphy, S ; Gomez, DE ; Mulvaney, P (AMER CHEMICAL SOC, 2018-06-28)
    We demonstrate using single molecule spectroscopy that inorganic CsPbI3 perovskite quantum dots (PQDs) undergo an irreversible, photoaccelerated reaction with water that results in a blue-shift of the photoluminescence (PL) and ultimately to complete quenching of the emission. We find that decomposition does not take place in the presence of oxygen alone but that it requires light and water. We also analyze the blinking for some stable PQDs and find a continuous distribution of emission states with a linear correlation between intensity and lifetime. We postulate that, in addition to charging and discharging processes, blinking arises from the activation and deactivation of nonradiative recombination centers in the PQDs.
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    Impact of Surface Functionalization on the Quantum Coherence of Nitrogen-Vacancy Centers in Nanodiamonds
    Ryan, RG ; Stacey, A ; O'Donnell, KM ; Ohshima, T ; Johnson, BC ; Hollenberg, LCL ; Mulvaney, P ; Simpson, DA (AMER CHEMICAL SOC, 2018-04-18)
    Nanoscale quantum probes such as the nitrogen-vacancy (NV) center in diamonds have demonstrated remarkable sensing capabilities over the past decade as control over fabrication and manipulation of these systems has evolved. The biocompatibility and rich surface chemistry of diamonds has added to the utility of these probes but, as the size of these nanoscale systems is reduced, the surface chemistry of diamond begins to impact the quantum properties of the NV center. In this work, we systematically study the effect of the diamond surface chemistry on the quantum coherence of the NV center in nanodiamonds (NDs) 50 nm in size. Our results show that a borane-reduced diamond surface can on average double the spin relaxation time of individual NV centers in nanodiamonds when compared to thermally oxidized surfaces. Using a combination of infrared and X-ray absorption spectroscopy techniques, we correlate the changes in quantum relaxation rates with the conversion of sp2 carbon to C-O and C-H bonds on the diamond surface. These findings implicate double-bonded carbon species as a dominant source of spin noise for near surface NV centers. The link between the surface chemistry and quantum coherence indicates that through tailored engineering of the surface, the quantum properties and magnetic sensitivity of these nanoscale systems may approach that observed in bulk diamond.
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    Vortex lattice formation in dipolar Bose-Einstein condensates via rotation of the polarization
    Prasad, SB ; Bland, T ; Mulkerin, BC ; Parker, NG ; Martin, AM (AMER PHYSICAL SOC, 2019-08-26)
    The behavior of a harmonically trapped dipolar Bose-Einstein condensate with its dipole moments rotating at angular frequencies lower than the transverse harmonic trapping frequency is explored in the co-rotating frame. We obtain semi-analytical solutions for the stationary states in the Thomas-Fermi limit of the corresponding dipolar Gross-Pitaevskii equation and utilize linear stability analysis to elucidate a phase diagram for the dynamical stability of these stationary solutions with respect to collective modes. These results are verified via direct numerical simulations of the dipolar Gross-Pitaevskii equation, which demonstrate that dynamical instabilities of the co-rotating stationary solutions lead to the seeding of vortices that eventually relax into a triangular lattice configuration. Our results illustrate that rotation of the dipole polarization represents a new route to vortex formation in dipolar Bose-Einstein condensates.
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    Discovery of processive catalysis by an exo-hydrolase with a pocket-shaped active site.
    Streltsov, VA ; Luang, S ; Peisley, A ; Varghese, JN ; Ketudat Cairns, JR ; Fort, S ; Hijnen, M ; Tvaroška, I ; Ardá, A ; Jiménez-Barbero, J ; Alfonso-Prieto, M ; Rovira, C ; Mendoza, F ; Tiessler-Sala, L ; Sánchez-Aparicio, J-E ; Rodríguez-Guerra, J ; Lluch, JM ; Maréchal, J-D ; Masgrau, L ; Hrmova, M (Springer Science and Business Media LLC, 2019-05-20)
    Substrates associate and products dissociate from enzyme catalytic sites rapidly, which hampers investigations of their trajectories. The high-resolution structure of the native Hordeum exo-hydrolase HvExoI isolated from seedlings reveals that non-covalently trapped glucose forms a stable enzyme-product complex. Here, we report that the alkyl β-D-glucoside and methyl 6-thio-β-gentiobioside substrate analogues perfused in crystalline HvExoI bind across the catalytic site after they displace glucose, while methyl 2-thio-β-sophoroside attaches nearby. Structural analyses and multi-scale molecular modelling of nanoscale reactant movements in HvExoI reveal that upon productive binding of incoming substrates, the glucose product modifies its binding patterns and evokes the formation of a transient lateral cavity, which serves as a conduit for glucose departure to allow for the next catalytic round. This path enables substrate-product assisted processive catalysis through multiple hydrolytic events without HvExoI losing contact with oligo- or polymeric substrates. We anticipate that such enzyme plasticity could be prevalent among exo-hydrolases.
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    Angular-momentum nanometrology in an ultrathin plasmonic topological insulator film.
    Yue, Z ; Ren, H ; Wei, S ; Lin, J ; Gu, M (Springer Science and Business Media LLC, 2018-10-24)
    Complementary metal-oxide-semiconductor (CMOS) technology has provided a highly sensitive detection platform for high-resolution optical imaging, sensing and metrology. Although the detection of optical beams carrying angular momentum have been explored with nanophotonic methods, the metrology of optical angular momentum has been limited to bulk optics. We demonstrate angular-momentum nanometrology through the spatial displacement engineering of plasmonic angular momentum modes in a CMOS-compatible plasmonic topological insulator material. The generation and propagation of surface plasmon polaritons on the surface of an ultrathin topological insulator Sb2Te3 film with a thickness of 100 nm is confirmed, exhibiting plasmonic figures of merit superior to noble metal plasmonics in the ultraviolet-visible frequency range. Angular-momentum nanometrology with a low crosstalk of less than -20 dB is achieved. This compact high-precision angular-momentum nanometrology opens an unprecedented opportunity for on-chip manipulation of optical angular momentum for high-capacity information processing, ultrasensitive molecular sensing, and ultracompact multi-functional optoelectronic devices.
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    Toward broadband, dynamic structuring of a complex plasmonic field
    Wei, S ; Si, G ; Malek, M ; Earl, SK ; Du, L ; Kou, SS ; Yuan, X ; Lin, J (AMER ASSOC ADVANCEMENT SCIENCE, 2018-06)
    The ability to tailor a coherent surface plasmon polariton (SPP) field is an important step toward many new opportunities for a broad range of nanophotonic applications. Previously, both scanning a converging SPP spot and designing SPP profiles using an ensemble of spots have been demonstrated. SPPs, however, are normally excited by intense, coherent light sources, that is, lasers. Hence, interference between adjacent spots is inevitable and will affect the overall SPP field distributions. We report a reconfigurable and wavelength-independent platform for generating a tailored two-dimensional (2D) SPP field distribution by considering the coherent field as a whole rather than as individual spots. With this new approach, the inherent constraints in a 2D coherent field distribution are revealed. Our design approach works not only for SPP waves but also for other 2D wave systems such as surface acoustic waves.
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    Discovery of a Powerful >10^61 erg AGN Outburst in Distant Galaxy Cluster SPT-CLJ0528-5300
    Calzadilla, MS ; McDonald, M ; Bayliss, M ; Benson, BA ; Bleem, LE ; Brodwin, M ; Edge, AC ; Floyd, B ; Gupta, N ; Hlavacek-Larrondo, J ; McNamara, BR ; Reichardt, CL ( 2019-11-28)
    We present ∼103 ks of Chandra observations of the galaxy cluster SPT-CLJ0528-5300 (SPT0528, z = 0.768). This cluster harbors the most radio-loud (L1.4GHz = 1.01 × 1033 erg s−1 Hz−1) central active galactic nucleus (AGN) of any cluster in the South Pole Telescope (SPT) Sunyaev–Zeldovich survey with available X-ray data. We find evidence of AGN-inflated cavities in the X-ray emission, which are consistent with the orientation of the jet direction revealed by Australia Telescope Compact Array radio data. The combined probability that two such depressions—each at ∼1.4–1.8σ significance, oriented ∼180° apart and aligned with the jet axis—would occur by chance is 0.1%. At ≳1061 erg, the outburst in SPT0528 is among the most energetic known in the universe, and certainly the most powerful known at z > 0.25. This work demonstrates that such powerful outbursts can be detected even in shallow X-ray exposures out to relatively high redshifts (z ∼ 0.8), providing an avenue for studying the evolution of extreme AGN feedback. The ratio of the cavity power (${P}_{\mathrm{cav}}=(9.4\pm 5.8)\times {10}^{45}$ erg s−1) to the cooling luminosity (Lcool = (1.5 ± 0.5) × 1044 erg s−1) for SPT0528 is among the highest measured to date. If, in the future, additional systems are discovered at similar redshifts with equally high Pcav/Lcool ratios, it would imply that the feedback/cooling cycle was not as gentle at high redshifts as in the low-redshift universe.
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    Dark Energy Survey year 1 results: Joint analysis of galaxy clustering, galaxy lensing, and CMB lensing two-point functions
    Abbott, TMC ; Abdalla, FB ; Alarcon, A ; Allam, S ; Annis, J ; Avila, S ; Aylor, K ; Banerji, M ; Banik, N ; Baxter, EJ ; Bechtol, K ; Becker, MR ; Benson, BA ; Bernstein, GM ; Bertin, E ; Bianchini, F ; Blazek, J ; Bleem, LE ; Bridle, SL ; Brooks, D ; Buckley-Geer, E ; Burke, DL ; Carlstrom, JE ; Rosell, AC ; Kind, MC ; Carretero, J ; Castander, FJ ; Cawthon, R ; Chang, C ; Chang, CL ; Cho, H-M ; Choi, A ; Chown, R ; Crawford, TM ; Crites, AT ; Crocce, M ; Cunha, CE ; D'Andrea, CB ; da Costa, LN ; Davis, C ; de Haan, T ; DeRose, J ; Desai, S ; De Vicente, J ; Diehl, HT ; Dietrich, JP ; Dobbs, MA ; Dodelson, S ; Doel, P ; Drlica-Wagner, A ; Eifler, TF ; Elvin-Poole, J ; Everett, WB ; Flaugher, B ; Fosalba, P ; Friedrich, O ; Frieman, J ; Garcia-Bellido, J ; Gatti, M ; Gaztanaga, E ; George, EM ; Gerdes, DW ; Giannantonio, T ; Gruen, D ; Gruendl, RA ; Gschwend, J ; Gutierrez, G ; Halverson, NW ; Harrington, NL ; Hartley, WG ; Holder, GP ; Hollowood, DL ; Holzapfel, WL ; Honscheid, K ; Hou, Z ; Hoyle, B ; Hrubes, JD ; Huterer, D ; Jain, B ; James, DJ ; Jarvis, M ; Jeltema, T ; Johnson, MWG ; Johnson, MD ; Kent, S ; Kirk, D ; Knox, L ; Kokron, N ; Krause, E ; Kuehn, K ; Lahav, O ; Lee, AT ; Leitch, EM ; Li, TS ; Lima, M ; Lin, H ; Luong-Van, D ; MacCrann, N ; Maia, MAG ; Manzotti, A ; Marrone, DP ; Marshall, JL ; Martini, P ; McMahon, JJ ; Menanteau, F ; Meyer, SS ; Miquel, R ; Mocanu, LM ; Mohr, JJ ; Muir, J ; Natoli, T ; Nicola, A ; Nord, B ; Omori, Y ; Padin, S ; Pandey, S ; Plazas, AA ; Porredon, A ; Prat, J ; Pryke, C ; Rau, MM ; Reichardt, CL ; Rollins, RP ; Romer, AK ; Roodman, A ; Ross, AJ ; Rozo, E ; Ruhl, JE ; Rykoff, ES ; Samuroff, S ; Sanchez, C ; Sanchez, E ; Sayre, JT ; Scarpine, V ; Schaffer, KK ; Secco, LF ; Serrano, S ; Sevilla-Noarbe, I ; Sheldon, E ; Shirokoff, E ; Simard, G ; Smith, M ; Soares-Santos, M ; Sobreira, F ; Staniszewski, Z ; Stark, AA ; Story, KT ; Suchyta, E ; Swanson, MEC ; Tarle, G ; Thomas, D ; Troxel, MA ; Tucker, DL ; Vanderlinde, K ; Vieira, JD ; Vielzeuf, P ; Vikram, V ; Walker, AR ; Wechsler, RH ; Weller, J ; Williamson, R ; Wu, WLK ; Yanny, B ; Zahn, O ; Zhang, Y ; Zuntz, J (AMER PHYSICAL SOC, 2019-07-26)
    We perform a joint analysis of the auto and cross-correlations between three cosmic fields: the galaxy density field, the galaxy weak lensing shear field, and the cosmic microwave background (CMB) weak lensing convergence field. These three fields are measured using roughly 1300 sq. deg. of overlapping optical imaging data from first year observations of the Dark Energy Survey (DES) and millimeter-wave observations of the CMB from both the South Pole Telescope Sunyaev-Zel’dovich survey and Planck. We present cosmological constraints from the joint analysis of the two-point correlation functions between galaxy density and galaxy shear with CMB lensing. We test for consistency between these measurements and the DES-only two-point function measurements, finding no evidence for inconsistency in the context of flat ΛCDM cosmological models. Performing a joint analysis of five of the possible correlation functions between these fields (excluding only the CMB lensing autospectrum) yields S8≡σ8√Ωm/0.3=0.782+0.019−0.025 and Ωm=0.260+0.029−0.019. We test for consistency between these five correlation function measurements and the Planck-only measurement of the CMB lensing autospectrum, again finding no evidence for inconsistency in the context of flat ΛCDM models. Combining constraints from all six two-point functions yields S8=0.776+0.014−0.021 and Ωm=0.271+0.022−0.016. These results provide a powerful test and confirmation of the results from the first year DES joint-probes analysis.
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    Cosmological lensing ratios with DES Y1, SPT, and Planck
    Prat, J ; Baxter, E ; Shin, T ; Sanchez, C ; Chang, C ; Jain, B ; Miquel, R ; Alarcon, A ; Bacon, D ; Bernstein, GM ; Cawthon, R ; Crawford, TM ; Davis, C ; De Vicente, J ; Dodelson, S ; Eifler, TF ; Friedrich, O ; Gatti, M ; Gruen, D ; Hartley, WG ; Holder, GP ; Hoyle, B ; Jarvis, M ; Krause, E ; MacCrann, N ; Mawdsley, B ; Nicola, A ; Omori, Y ; Pujol, A ; Rau, MM ; Reichardt, CL ; Samuroff, S ; Sheldon, E ; Troxel, MA ; Vielzeuf, P ; Zuntz, J ; Abbott, TMC ; Abdalla, FB ; Annis, J ; Avila, S ; Aylor, K ; Benson, BA ; Bertin, E ; Bleem, LE ; Brooks, D ; Burke, DL ; Carlstrom, JE ; Kind, MC ; Carretero, J ; Chang, CL ; Cho, H-M ; Chown, R ; Crites, AT ; Cunha, CE ; da Costa, LN ; Desai, S ; Diehl, HT ; Dietrich, JP ; Dobbs, MA ; Doel, P ; Everett, WB ; Evrard, AE ; Flaugher, B ; Fosalba, P ; Garcia-Bellido, J ; Gaztanaga, E ; George, EM ; Gerdes, DW ; Giannantonio, T ; Gruendl, RA ; Gschwend, J ; Gutierrez, G ; de Haan, T ; Halverson, NW ; Harrington, NL ; Holzapfel, WL ; Honscheid, K ; Hou, Z ; Hrubes, JD ; James, DJ ; Jeltema, T ; Knox, L ; Kron, R ; Kuehn, K ; Kuropatkin, N ; Lahav, O ; Lee, AT ; Leitch, EM ; Lima, M ; Luong-Van, D ; Maia, MAG ; Manzotti, A ; Marrone, DP ; Marshall, JL ; McMahon, JJ ; Melchior, P ; Menanteau, F ; Meyer, SS ; Miller, CJ ; Mocanu, LM ; Mohr, JJ ; Natoli, T ; Padin, S ; Plazas, AA ; Pryke, C ; Romer, AK ; Roodman, A ; Ruhl, JE ; Rykoff, ES ; Sanchez, E ; Sayre, JT ; Scarpine, V ; Schaffer, KK ; Serrano, S ; Sevilla-Noarbe, I ; Shirokoff, E ; Simard, G ; Smith, M ; Soares-Santos, M ; Sobreira, F ; Staniszewski, Z ; Stark, AA ; Story, KT ; Suchyta, E ; Swanson, MEC ; Tarle, G ; Thomas, D ; Vanderlinde, K ; Vieira, JD ; Vikram, V ; Walker, AR ; Weller, J ; Williamson, R ; Zahn, O (OXFORD UNIV PRESS, 2019-07)
    ABSTRACT Correlations between tracers of the matter density field and gravitational lensing are sensitive to the evolution of the matter power spectrum and the expansion rate across cosmic time. Appropriately defined ratios of such correlation functions, on the other hand, depend only on the angular diameter distances to the tracer objects and to the gravitational lensing source planes. Because of their simple cosmological dependence, such ratios can exploit available signal-to-noise ratio down to small angular scales, even where directly modelling the correlation functions is difficult. We present a measurement of lensing ratios using galaxy position and lensing data from the Dark Energy Survey, and CMB lensing data from the South Pole Telescope and Planck, obtaining the highest precision lensing ratio measurements to date. Relative to the concordance ΛCDM model, we find a best-fitting lensing ratio amplitude of A = 1.1 ± 0.1. We use the ratio measurements to generate cosmological constraints, focusing on the curvature parameter. We demonstrate that photometrically selected galaxies can be used to measure lensing ratios, and argue that future lensing ratio measurements with data from a combination of LSST and Stage-4 CMB experiments can be used to place interesting cosmological constraints, even after considering the systematic uncertainties associated with photometric redshift and galaxy shear estimation.