Abstract <p>The influence of formation of thin layers of CdTe and ZnTe on the shape of instrument plates (IPs) has been clarified. In the process of formation of thin buffer layers of ZnTe (with a thickness of <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(20{-}300\)</EquationSource> <!--OptelIns2570010Novoselov-m1--> </InlineEquation> nm) and CdTe (<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(5{-}7\)</EquationSource> <!--OptelIns2570010Novoselov-m2--> </InlineEquation> <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570010Novoselov-m3--> </InlineEquation>m) on a GaAs IP (with a thickness of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\({\sim}420\)</EquationSource> <!--OptelIns2570010Novoselov-m4--> </InlineEquation> <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570010Novoselov-m5--> </InlineEquation>m), their bending increased by more than 1 <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570010Novoselov-m6--> </InlineEquation>m. A technological solution has been found to reduce the bending of GaAs instrument plates by more than 1 <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570010Novoselov-m7--> </InlineEquation>m after formation of thin layers (CdTe and ZnTe) after technological annealing at a temperature of 600<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11974_2025_8432_Article_IEq8.gif" Format="GIF" Height="7" Rendition="HTML" Resolution="72" Type="Linedraw" Width="9" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{\circ}\)</EquationSource> <!--OptelIns2570010Novoselov-m8--> </InlineEquation>C in high vacuum, slow cooling of the specimen (at a cooling rate of 0.5 deg/min) is carried out during 11 h.</p>

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Effect of Thin Layers of CdTe and ZnTe on the Shape of GaAs Substrates

  • A. R. Novoselov,
  • N. N. Mikhailov,
  • R. V. Menshchikov,
  • P. A. Aldokhin,
  • A. E. Matochkin

摘要

Abstract

The influence of formation of thin layers of CdTe and ZnTe on the shape of instrument plates (IPs) has been clarified. In the process of formation of thin buffer layers of ZnTe (with a thickness of \(20{-}300\) nm) and CdTe ( \(5{-}7\) \(\mu\) m) on a GaAs IP (with a thickness of \({\sim}420\) \(\mu\) m), their bending increased by more than 1 \(\mu\) m. A technological solution has been found to reduce the bending of GaAs instrument plates by more than 1 \(\mu\) m after formation of thin layers (CdTe and ZnTe) after technological annealing at a temperature of 600 \({}^{\circ}\) C in high vacuum, slow cooling of the specimen (at a cooling rate of 0.5 deg/min) is carried out during 11 h.