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Dawel F, Wilzewski A, Herbers S, Pelzer L, Kramer J, Hild MB, Dietze K, Krinner L, Spethmann NCH, Schmidt PO. Coherent photo-thermal noise cancellation in a dual-wavelength optical cavity for narrow-linewidth laser frequency stabilisation. OPTICS EXPRESS 2024; 32:7276-7288. [PMID: 38439412 DOI: 10.1364/oe.516433] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Academic Contribution Register] [Received: 12/21/2023] [Accepted: 02/01/2024] [Indexed: 03/06/2024]
Abstract
Optical resonators are used for the realisation of ultra-stable frequency lasers. The use of high reflectivity multi-band coatings allows the frequency locking of several lasers of different wavelengths to a single cavity. While the noise processes for single wavelength cavities are well known, the correlation caused by multi-stack coatings has as yet not been analysed experimentally. In our work, we stabilise the frequency of a 729 nm and a 1069 nm laser to one mirror pair and determine the residual-amplitude modulation (RAM) and photo-thermal noise (PTN). We find correlations in PTN between the two lasers and observe coherent cancellation of PTN for the 1069 nm coating. We show that the fractional frequency instability of the 729 nm laser is limited by RAM at 1 × 10-14. The instability of the 1069 nm laser is at 3 × 10-15 close to the thermal noise limit of 1.5 × 10-15.
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Molina-Ruiz M, Markosyan A, Bassiri R, Fejer MM, Abernathy M, Metcalf TH, Liu X, Vajente G, Ananyeva A, Hellman F. Hydrogen-Induced Ultralow Optical Absorption and Mechanical Loss in Amorphous Silicon for Gravitational-Wave Detectors. PHYSICAL REVIEW LETTERS 2023; 131:256902. [PMID: 38181375 DOI: 10.1103/physrevlett.131.256902] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Academic Contribution Register] [Received: 06/16/2023] [Revised: 10/31/2023] [Accepted: 11/22/2023] [Indexed: 01/07/2024]
Abstract
The sensitivity of gravitational-wave detectors is limited by the mechanical loss associated with the amorphous coatings of the detectors' mirrors. Amorphous silicon has higher refraction index and lower mechanical loss than current high-index coatings, but its optical absorption at the wavelength used for the detectors is at present large. The addition of hydrogen to the amorphous silicon network reduces both optical absorption and mechanical loss for films prepared under a range of conditions at all measured wavelengths and temperatures, with a particularly large effect on films grown at room temperature. The uptake of hydrogen is greatest in the films grown at room temperature, but still below 1.5 at.% H, which show an ultralow optical absorption (below 10 ppm) measured at 2000 nm for 500-nm-thick films. These results show that hydrogenation is a promising strategy to reduce both optical absorption and mechanical loss in amorphous silicon, and may enable fabrication of mirror coatings for gravitational-wave detectors with improved sensitivity.
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Affiliation(s)
- M Molina-Ruiz
- Department of Physics, University of California, Berkeley, California 94720, USA
| | - A Markosyan
- Edward L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - R Bassiri
- Edward L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - M M Fejer
- Edward L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - M Abernathy
- Naval Research Laboratory, Code 7130, Washington, DC 20375, USA
| | - T H Metcalf
- Naval Research Laboratory, Code 7130, Washington, DC 20375, USA
| | - X Liu
- Naval Research Laboratory, Code 7130, Washington, DC 20375, USA
| | - G Vajente
- LIGO Laboratory, California Institute of Technology, Pasadena, California 91125, USA
| | - A Ananyeva
- LIGO Laboratory, California Institute of Technology, Pasadena, California 91125, USA
| | - F Hellman
- Department of Physics, University of California, Berkeley, California 94720, USA
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Li W, Li X, Zhang X, Yu H, Han F, Bergara A, Lin J, Wu J, Yang G. Emergent superconductivity in TaO 3 at high pressures. Phys Chem Chem Phys 2023; 25:23502-23509. [PMID: 37624051 DOI: 10.1039/d3cp03094f] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Academic Contribution Register] [Indexed: 08/26/2023]
Abstract
Tantalum (Ta) is an interesting transition metal that exhibits superconductivity in its elemental states. Additionally, several Ta chalcogenides (S and Se) have also demonstrated superconducting properties. In this work, we propose the existence of five high-pressure metallic Ta-O compounds (e.g., TaO3, TaO2, TaO, Ta2O, and Ta3O), composed of polyhedra centered on Ta/O atoms. These compounds exhibit distinct characteristics compared to the well-known semiconducting Ta2O5. One particularly interesting finding is that TaO3 shows an estimated superconducting transition temperature (Tc) of 3.87 K at 200 GPa. This superconductivity is primarily driven by the coupling between the low-frequency phonons derived from Ta and the O 2p and Ta 5d electrons. Remarkably, its dynamically stabilized pressure can be as low as 50 GPa, resulting in an enhanced electron-phonon coupling and a higher Tc of up to 9.02 K. When compared to the superconductivity of isomorphic TaX3 (X = O, S, and Se) compounds, the highest Tc in TaO3 is associated with the highest NEF and phonon vibrational frequency. These characteristics arise from the strong electronegativity and small atomic mass of the O atom. Consequently, our findings offer valuable insights into the intrinsic physical mechanisms of high-pressure behaviors in Ta-O compounds.
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Affiliation(s)
- Wenjing Li
- Centre for Advanced Optoelectronic Functional Materials Research and Key Laboratory for UV Light-Emitting Materials and Technology of Northeast Normal University, Changchun 130024, China.
| | - Xing Li
- State Key Laboratory of Metastable Materials Science & Technology and Key Laboratory for Microstructural Material Physics of Hebei Province, School of Science, Yanshan University, Qinhuangdao 066004, China
| | - Xiaohua Zhang
- State Key Laboratory of Metastable Materials Science & Technology and Key Laboratory for Microstructural Material Physics of Hebei Province, School of Science, Yanshan University, Qinhuangdao 066004, China
| | - Hong Yu
- Centre for Advanced Optoelectronic Functional Materials Research and Key Laboratory for UV Light-Emitting Materials and Technology of Northeast Normal University, Changchun 130024, China.
| | - Fanjunjie Han
- Centre for Advanced Optoelectronic Functional Materials Research and Key Laboratory for UV Light-Emitting Materials and Technology of Northeast Normal University, Changchun 130024, China.
| | - Aitor Bergara
- Departamento de Física, Universidad del País Vasco-Euskal Herriko Unibertsitatea, UPV/EHU, Bilbao 48080, Spain.
- Donostia International Physics Center (DIPC), Donostia 20018, Spain
- Centro de Física de Materiales CFM, Centro Mixto CSIC-UPV/EHU, Donostia 20018, Spain
| | - Jianyan Lin
- College of Physics, Changchun Normal University, Changchun 130032, China.
| | - Jinhui Wu
- Centre for Advanced Optoelectronic Functional Materials Research and Key Laboratory for UV Light-Emitting Materials and Technology of Northeast Normal University, Changchun 130024, China.
| | - Guochun Yang
- Centre for Advanced Optoelectronic Functional Materials Research and Key Laboratory for UV Light-Emitting Materials and Technology of Northeast Normal University, Changchun 130024, China.
- State Key Laboratory of Metastable Materials Science & Technology and Key Laboratory for Microstructural Material Physics of Hebei Province, School of Science, Yanshan University, Qinhuangdao 066004, China
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