Approximating the incoming stimulus arising from the sensory neurons as a Gaussian in both space and time. Such a stimulus has the normalized form \begin{eqnarray} &&\phi_n({\bf{r}}, t)=\frac{{\text e}^{-\frac{1}{2}\left(\frac{t-t_{os}}{t_s}\right)^2}}{t_s\sqrt(2\pi)}\frac{{\text e}^{\left(\frac{\left|{\bf r}-{{\bf r}_{os}}\right|}{r_s}\right)^2}}{\pi r_s^2}. \end{eqnarray} where $t_s$ is the characteristics duaration of the stimulus, $t_{os}$ is the transmission delay from cochlea to thalamus, $r_s$ is the spatial width of the stimulus at cortex, and $\bf r_{os}$ is the offset of the centre of the stimulus from the point of measurement. The Fourier transform of this function is \begin{eqnarray} \phi_n({\bf{k}}, \omega)&&={\text{e}}^{-\frac{1}{2}\omega^2 t_s^2}{\text{e}}^{i \omega t_{os}}{\text {e}}^{-(\frac{kr_s}{2})^2}{\text {e}}^{{{\text{i}}\bf{k}.\bf{r_{os}}}} \end{eqnarray} Can anyone please help me to show every step to find the Fourier transform of this function? Thanks in advance!
2026-03-28 16:56:32.1774716992
Fourier Transform of Gaussian function
780 Views Asked by Bumbble Comm https://math.techqa.club/user/bumbble-comm/detail At
1
There are 1 best solutions below
Related Questions in FOURIER-TRANSFORM
- Proof of Fourier transform of cos$2\pi ft$
- Find the convergence of series of a sequence of functions in $L^2(\mathbb{R})$
- solving a simple ODE with Fourier transform
- How can we prove that $e^{-jωn}$ converges at $0$ while n -> infinity?
- Show that a periodic function $f(t)$ with period $T$ can be written as $ f(t) = f_T (t) \star \frac{1}{T} \text{comb}\bigg(\frac{t}{T}\bigg) $
- Taking the Discrete Inverse Fourier Transform of a Continuous Forward Transform
- Arcsin of a number greater than one
- Complex numbers in programming
- Power spectrum of field over an arbitrarily-shaped country
- Computing an inverse Fourier Transform / Solving the free particle Schrödinger equation with a gaussian wave packet as initial condition
Related Questions in GAUSSIAN-INTEGRAL
- Evaluating $\int_{\mathbb{R}}e^{-(x+iy)^2}dx$? For a fixed $y \in \mathbb{R}$,
- How to calculate $\iint_{\mathbb{R}^2} \exp\left(-x^2-y^2+ixy-ix-iy\right)\,dx\,dy$?
- Fourier transform of squared Gaussian Hermite polynomial
- Formal derivation of the Fourier transform of Dirac delta using a distribution
- Why Owen's selected this function $f(h,x)=\frac{e^{-\frac 12 h^2(1+x²)}}{1+x²}$ for integration?
- Calculate $\int_{\mathbb R^3} \exp(-x^tAx + b^tx) \,\lambda_3(dx)$
- Complex Gaussian integral
- How do I perform the following integral involving two vector coordinates?
- Can the following integral be solved exactly without approximation ? if so how to evaluate?
- Is this possible to solve this definite integral?
Trending Questions
- Induction on the number of equations
- How to convince a math teacher of this simple and obvious fact?
- Find $E[XY|Y+Z=1 ]$
- Refuting the Anti-Cantor Cranks
- What are imaginary numbers?
- Determine the adjoint of $\tilde Q(x)$ for $\tilde Q(x)u:=(Qu)(x)$ where $Q:U→L^2(Ω,ℝ^d$ is a Hilbert-Schmidt operator and $U$ is a Hilbert space
- Why does this innovative method of subtraction from a third grader always work?
- How do we know that the number $1$ is not equal to the number $-1$?
- What are the Implications of having VΩ as a model for a theory?
- Defining a Galois Field based on primitive element versus polynomial?
- Can't find the relationship between two columns of numbers. Please Help
- Is computer science a branch of mathematics?
- Is there a bijection of $\mathbb{R}^n$ with itself such that the forward map is connected but the inverse is not?
- Identification of a quadrilateral as a trapezoid, rectangle, or square
- Generator of inertia group in function field extension
Popular # Hahtags
second-order-logic
numerical-methods
puzzle
logic
probability
number-theory
winding-number
real-analysis
integration
calculus
complex-analysis
sequences-and-series
proof-writing
set-theory
functions
homotopy-theory
elementary-number-theory
ordinary-differential-equations
circles
derivatives
game-theory
definite-integrals
elementary-set-theory
limits
multivariable-calculus
geometry
algebraic-number-theory
proof-verification
partial-derivative
algebra-precalculus
Popular Questions
- What is the integral of 1/x?
- How many squares actually ARE in this picture? Is this a trick question with no right answer?
- Is a matrix multiplied with its transpose something special?
- What is the difference between independent and mutually exclusive events?
- Visually stunning math concepts which are easy to explain
- taylor series of $\ln(1+x)$?
- How to tell if a set of vectors spans a space?
- Calculus question taking derivative to find horizontal tangent line
- How to determine if a function is one-to-one?
- Determine if vectors are linearly independent
- What does it mean to have a determinant equal to zero?
- Is this Batman equation for real?
- How to find perpendicular vector to another vector?
- How to find mean and median from histogram
- How many sides does a circle have?
IMO one of the most intuitive proof is to set $$F(s) = \int_{-\infty}^\infty e^{-t^2} e^{-2st}dt, \qquad s \in \mathbb{C}$$ Assuming $s \in \mathbb{R}$ then $$F(s) = \int_{-\infty}^\infty e^{s^2} e^{-(t+s)^2}dt =e^{s^2}\int_{-\infty}^\infty e^{-t^2}dt= e^{s^2} F(0)$$ And to convince yourself that $F(s)-e^{s^2}F(0)=0$ stays true for every $s \in \mathbb{C}$, because both sides are complex analytic functions of $s$ (a non-zero power series $\sum_{n=0}^\infty a_n s^n$ cannot vanish for every $s\in \mathbb{R}$).
Thus $\displaystyle\int_{-\infty}^\infty e^{-t^2}e^{-i \omega t}dt = F(i\omega/2)=e^{-(\omega/2)^2} F(0)$ and $$\int_{-\infty}^\infty\int_{-\infty}^\infty e^{-a^2(t+b)^2}e^{-c^2(r+d)^2}e^{-i k r}e^{-i \omega t}dtdr = \frac{1}{|a|}e^{-(\omega/2)^2/a^2} e^{-i \omega b}\frac{1}{|c|}e^{-(k/2)^2/c^2} e^{-i kd}F(0)^2$$ Finally by inverse Fourier transform we show $F(0) = \sqrt{\pi}$.