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   	<dc:title>Cryogenic electro-optic modulation in titanium in-diffused lithium niobate waveguides</dc:title>
   	<dc:creator>Thiele, Frederik</dc:creator>
   	<dc:creator>vom Bruch, Felix</dc:creator>
   	<dc:creator>Brockmeier, Julian</dc:creator>
   	<dc:creator>Protte, Maximilian</dc:creator>
   	<dc:creator>Hummel, Thomas</dc:creator>
   	<dc:creator>Ricken, Raimund</dc:creator>
   	<dc:creator>Quiring, Viktor</dc:creator>
   	<dc:creator>Lengeling, Sebastian</dc:creator>
   	<dc:creator>Herrmann, Harald</dc:creator>
   	<dc:creator>Eigner, Christof</dc:creator>
   	<dc:creator>Silberhorn, Christine</dc:creator>
   	<dc:creator>Bartley, Tim</dc:creator>
   	<dc:subject>Electrical and Electronic Engineering</dc:subject>
   	<dc:subject>Atomic and Molecular Physics</dc:subject>
   	<dc:subject>and Optics</dc:subject>
   	<dc:subject>Electronic</dc:subject>
   	<dc:subject>Optical and Magnetic Materials</dc:subject>
   	<dc:description>&lt;jats:title&gt;Abstract&lt;/jats:title&gt;
               &lt;jats:p&gt;Lithium niobate is a promising platform for integrated quantum optics. In this platform, we aim to efficiently manipulate and detect quantum states by combining superconducting single photon detectors and modulators. The cryogenic operation of a superconducting single photon detector dictates the optimisation of the electro-optic modulators under the same operating conditions. To that end, we characterise a phase modulator, directional coupler, and polarisation converter at both ambient and cryogenic temperatures. The operation voltage &lt;jats:inline-formula&gt;
                     &lt;jats:tex-math&gt;&lt;?CDATA $V_{\pi/2}$?&gt;&lt;/jats:tex-math&gt;
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                              &lt;mml:mrow&gt;
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                              &lt;/mml:mrow&gt;
                              &lt;mml:mn&gt;2&lt;/mml:mn&gt;
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                        &lt;/mml:msub&gt;
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                     &lt;jats:inline-graphic xmlns:xlink=&quot;http://www.w3.org/1999/xlink&quot; xlink:href=&quot;jpphotonac6c63ieqn1.gif&quot; xlink:type=&quot;simple&quot; /&gt;
                  &lt;/jats:inline-formula&gt; of these modulators increases, due to the decrease in the electro-optic effect, by 74% for the phase modulator, 84% for the directional coupler and 35% for the polarisation converter below 8.5&lt;jats:inline-formula&gt;
                     &lt;jats:tex-math&gt;&lt;?CDATA $\,\mathrm{K}$?&gt;&lt;/jats:tex-math&gt;
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                     &lt;jats:inline-graphic xmlns:xlink=&quot;http://www.w3.org/1999/xlink&quot; xlink:href=&quot;jpphotonac6c63ieqn2.gif&quot; xlink:type=&quot;simple&quot; /&gt;
                  &lt;/jats:inline-formula&gt;. The phase modulator preserves its broadband nature and modulates light in the characterised wavelength range. The unbiased bar state of the directional coupler changed by a wavelength shift of 85&lt;jats:inline-formula&gt;
                     &lt;jats:tex-math&gt;&lt;?CDATA $\,\mathrm{nm}$?&gt;&lt;/jats:tex-math&gt;
                     &lt;mml:math xmlns:mml=&quot;http://www.w3.org/1998/Math/MathML&quot; overflow=&quot;scroll&quot;&gt;
                        &lt;mml:mrow&gt;
                           &lt;mml:mi mathvariant=&quot;normal&quot;&gt;n&lt;/mml:mi&gt;
                           &lt;mml:mi mathvariant=&quot;normal&quot;&gt;m&lt;/mml:mi&gt;
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                  &lt;/jats:inline-formula&gt; while cooling the device down to 5&lt;jats:inline-formula&gt;
                     &lt;jats:tex-math&gt;&lt;?CDATA $\,\mathrm{K}$?&gt;&lt;/jats:tex-math&gt;
                     &lt;mml:math xmlns:mml=&quot;http://www.w3.org/1998/Math/MathML&quot; overflow=&quot;scroll&quot;&gt;
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                     &lt;jats:inline-graphic xmlns:xlink=&quot;http://www.w3.org/1999/xlink&quot; xlink:href=&quot;jpphotonac6c63ieqn4.gif&quot; xlink:type=&quot;simple&quot; /&gt;
                  &lt;/jats:inline-formula&gt;. The polarisation converter uses periodic poling to phasematch the two orthogonal polarisations. The phasematched wavelength of the utilised poling changes by 112&lt;jats:inline-formula&gt;
                     &lt;jats:tex-math&gt;&lt;?CDATA $\,\mathrm{nm}$?&gt;&lt;/jats:tex-math&gt;
                     &lt;mml:math xmlns:mml=&quot;http://www.w3.org/1998/Math/MathML&quot; overflow=&quot;scroll&quot;&gt;
                        &lt;mml:mrow&gt;
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                  &lt;/jats:inline-formula&gt; when cooling to 5&lt;jats:inline-formula&gt;
                     &lt;jats:tex-math&gt;&lt;?CDATA $\,\mathrm{K}$?&gt;&lt;/jats:tex-math&gt;
                     &lt;mml:math xmlns:mml=&quot;http://www.w3.org/1998/Math/MathML&quot; overflow=&quot;scroll&quot;&gt;
                        &lt;mml:mrow&gt;
                           &lt;mml:mi mathvariant=&quot;normal&quot;&gt;K&lt;/mml:mi&gt;
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                  &lt;/jats:inline-formula&gt;.&lt;/jats:p&gt;</dc:description>
   	<dc:publisher>IOP Publishing</dc:publisher>
   	<dc:date>2022</dc:date>
   	<dc:type>info:eu-repo/semantics/article</dc:type>
   	<dc:type>doc-type:article</dc:type>
   	<dc:type>text</dc:type>
   	<dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
   	<dc:identifier>https://ris.uni-paderborn.de/record/33672</dc:identifier>
   	<dc:source>Thiele F, vom Bruch F, Brockmeier J, et al. Cryogenic electro-optic modulation in titanium in-diffused lithium niobate waveguides. &lt;i&gt;Journal of Physics: Photonics&lt;/i&gt;. 2022;4(3). doi:&lt;a href=&quot;https://doi.org/10.1088/2515-7647/ac6c63&quot;&gt;10.1088/2515-7647/ac6c63&lt;/a&gt;</dc:source>
   	<dc:language>eng</dc:language>
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   	<dc:relation>info:eu-repo/semantics/altIdentifier/issn/2515-7647</dc:relation>
   	<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
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