<p>Einstein Telescope (ET) is expected to achieve sensitivity improvements exceeding an order of magnitude compared to current gravitational-wave detectors. The rigorous characterization in optical birefringence of materials and coatings has become a critical task for next-generation detectors, especially since this birefringence is generally spatially non-uniform. A highly sensitive optical polarimeter has been developed at the Department of Physics and Earth Sciences of the University of Ferrara and INFN - Ferrara Section, Italy, aimed at performing two-dimensional birefringence mapping of substrates. In this paper we describe the design and working principle of the system and present results for crystalline silicon, a candidate material for substrates in the low-frequency interferometers of ET. We find that the birefringence is <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\lesssim 10^{-7}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>≲</mo> <msup> <mn>10</mn> <mrow> <mo>-</mo> <mn>7</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> for commercially available samples and is position dependent in the silicon (100)-oriented samples, with variations in both magnitude and axis orientation. We also measure the intrinsic birefringence of the (110) surface: <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Delta n^{(110)}=-(1.50\pm 0.15)\times 10^{-6}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <msup> <mi>n</mi> <mrow> <mo stretchy="false">(</mo> <mn>110</mn> <mo stretchy="false">)</mo> </mrow> </msup> <mo>=</mo> <mo>-</mo> <mrow> <mo stretchy="false">(</mo> <mn>1.50</mn> <mo>±</mo> <mn>0.15</mn> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>-</mo> <mn>6</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> @ <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda =1550\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>=</mo> <mn>1550</mn> </mrow> </math></EquationSource> </InlineEquation>&#xa0;nm. Implications for the performance of gravitational-wave interferometers are discussed.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Apparatus for the measurement of birefringence maps of optical materials: the case of crystalline silicon for Einstein Telescope

  • Alina Mariana Soflau,
  • Federico Della Valle,
  • Francesco Cescato,
  • Giovanni Di Domenico,
  • Aurélie Max Mailliet,
  • Lorenzo Malagutti,
  • Emilio Mariotti,
  • Andrea Mazzolari,
  • Marco Romagnoni,
  • Guido Zavattini

摘要

Einstein Telescope (ET) is expected to achieve sensitivity improvements exceeding an order of magnitude compared to current gravitational-wave detectors. The rigorous characterization in optical birefringence of materials and coatings has become a critical task for next-generation detectors, especially since this birefringence is generally spatially non-uniform. A highly sensitive optical polarimeter has been developed at the Department of Physics and Earth Sciences of the University of Ferrara and INFN - Ferrara Section, Italy, aimed at performing two-dimensional birefringence mapping of substrates. In this paper we describe the design and working principle of the system and present results for crystalline silicon, a candidate material for substrates in the low-frequency interferometers of ET. We find that the birefringence is \(\lesssim 10^{-7}\) 10 - 7 for commercially available samples and is position dependent in the silicon (100)-oriented samples, with variations in both magnitude and axis orientation. We also measure the intrinsic birefringence of the (110) surface: \(\Delta n^{(110)}=-(1.50\pm 0.15)\times 10^{-6}\) Δ n ( 110 ) = - ( 1.50 ± 0.15 ) × 10 - 6 @ \(\lambda =1550\) λ = 1550  nm. Implications for the performance of gravitational-wave interferometers are discussed.