<p>In this paper, we propose a novel <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( n -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>Dimensional Pseudo-Differential Operator (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( n -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>DPDO) constructed using the robust framework of the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( n -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>Dimensional Quadratic Phase Fourier Transform (<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq1.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(n-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>DQPFT). This operator is characterized by a smooth symbol <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="282" /> </InlineMediaObject> <EquationSource Format="TEX">\( \delta (\nu _1, \dots , \nu _n; \omega _1, \dots , \omega _n) \in {\mathcal {C}}^\infty ({\mathbb {R}}^n \times {\mathbb {R}}^n) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>δ</mi> <mrow> <mo stretchy="false">(</mo> <msub> <mi>ν</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <msub> <mi>ν</mi> <mi>n</mi> </msub> <mo>;</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <msub> <mi>ω</mi> <mi>n</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mrow> <mi mathvariant="script">C</mi> </mrow> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, paving the way for new directions in mathematical analysis. We provide a rigorous study of its fundamental properties within the context of Schwartz space, proving that the composition of two <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( n -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>DPDOs yields another <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( n -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>DPDO, thereby establishing its algebraic consistency. Furthermore, we analyze formal adjoint operators with symbols in <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\( {\mathcal {S}}^r \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="script">S</mi> </mrow> <mi>r</mi> </msup> </math></EquationSource> </InlineEquation>, demonstrating their essential boundedness in <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\( L^p({\mathbb {R}}^n) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> spaces under the <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( n -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>DQPFT framework. Additionally, the <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11868_2025_688_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( n -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation>DQPFT is applied to solve generalized partial differential equations. Specific cases of these equations include well-known n-dimensional time-dependent generalized Schrödinger-type equations (Types I, II, and III) and the general Schrödinger equation in quantum mechanics for a single particle with a constant potential.</p>

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An \(n-\)dimensional pseudo-differential operator involving quadratic phase Fourier transform and applications in quantum mechanics

  • Manish Kumar,
  • Bhawna

摘要

In this paper, we propose a novel \( n -\) n - Dimensional Pseudo-Differential Operator ( \( n -\) n - DPDO) constructed using the robust framework of the \( n -\) n - Dimensional Quadratic Phase Fourier Transform ( \(n-\) n - DQPFT). This operator is characterized by a smooth symbol \( \delta (\nu _1, \dots , \nu _n; \omega _1, \dots , \omega _n) \in {\mathcal {C}}^\infty ({\mathbb {R}}^n \times {\mathbb {R}}^n) \) δ ( ν 1 , , ν n ; ω 1 , , ω n ) C ( R n × R n ) , paving the way for new directions in mathematical analysis. We provide a rigorous study of its fundamental properties within the context of Schwartz space, proving that the composition of two \( n -\) n - DPDOs yields another \( n -\) n - DPDO, thereby establishing its algebraic consistency. Furthermore, we analyze formal adjoint operators with symbols in \( {\mathcal {S}}^r \) S r , demonstrating their essential boundedness in \( L^p({\mathbb {R}}^n) \) L p ( R n ) spaces under the \( n -\) n - DQPFT framework. Additionally, the \( n -\) n - DQPFT is applied to solve generalized partial differential equations. Specific cases of these equations include well-known n-dimensional time-dependent generalized Schrödinger-type equations (Types I, II, and III) and the general Schrödinger equation in quantum mechanics for a single particle with a constant potential.