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Linear Integral Equations

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1. Fredholm and Volterra equations

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Lec-21 Calculus of Variations and Integral Equations

NPTEL · Calculus of Variations and Integral Equations

Integral equations begin here: Fredholm and Volterra, first and second kind.

Lec-22 Calculus of Variations and Integral Equations

NPTEL · Calculus of Variations and Integral Equations

Conversion between differential and integral equations.

Integral equations: Fredholm vs Volterra free

In plain words

Both have the unknown sitting inside an integral, and only the upper limit differs. A fixed limit brings eigenvalues and can fail. A moving limit always has exactly one solution.

The two types

  • Fredholm: y(x)=f(x)+λ∫ay(x) = f(x) + \lambda\int_{a}ᵇ K(x,t)y(t)dt — fixed limits.
  • Volterra: y(x)=f(x)+λ∫ay(x) = f(x) + \lambda\int_{a}ˣ K(x,t)y(t)dt — variable upper limit.

Second kind has y outside the integral; first kind does not (and is ill-posed).

Volterra

The Neumann series always converges: a Volterra equation of the second kind has a unique solution for every λ\lambda, with no eigenvalues. Converting to an ODE is usually fastest: differentiate and use y(a) = f(a).

Example. y = eˣ +∫0+ \int_{0}ˣ ((1+x2)/(1+t2))y((1+x^{2})/(1+t^{2}))y dt. Put I(x)=∫0I(x) = \int_{0}ˣ y/(1+t2)y/(1+t^{2}); then I′ − I = eˣ/(1+x2)/(1+x^{2}), giving I = eˣ arctan x and y = eˣ(1+(1+x2)(1 + (1+x^{2})arctan x).

Fredholm with a separable (degenerate) kernel

K(x,t)=∑ai(x)bi(t)K(x,t) = \sum a_{i}(x)b_{i}(t) reduces the equation to a finite linear system. Eigenvalues are where that system is singular.

Example. K = xt on [0,1]:y=f+λx∫01ty[0,1]: y = f + \lambda{}x\int_{0}^{1} t y dt. Setting c=∫c = \intty gives c(1−λ/3)=∫c(1 - \lambda/3) = \inttf, so λ=3\lambda = 3 is the eigenvalue.

Fredholm alternative

For y−λ∫y - \lambda\intKy = f with λ\lambda an eigenvalue:

  • a solution exists iff f is orthogonal to every solution of the homogeneous adjoint equation;
  • then the solution is not unique (add any eigenfunction).

If λ\lambda is not an eigenvalue, there is a unique solution for every f.

Example. y−3∫01y - 3\int_{0}^{1} tx y dt = f is solvable iff ∫01tf(t)\int_{0}^{1} t f(t) dt = 0 — true for f=x2−f = x^{2} - ½ and f = 2 − 3x, false for eˣ and x − 1.

Relation to ODE

A boundary value problem converts to a Fredholm equation with the Green's function as kernel; an initial value problem converts to a Volterra equation.

Key takeaways

  • Volterra: always uniquely solvable. Fredholm: check for eigenvalues first.
  • Separable kernels reduce everything to linear algebra.
  • The alternative's solvability test is an orthogonality condition on f.

Volterra always solvable, Fredholm not — and whyinteractive

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The factorial in the iterated kernel that makes one type unconditionally well behaved.

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Exam focus: Volterra always has a unique solution; Fredholm depends on whether λ is an eigenvalue, and then the alternative decides solvability by an orthogonality condition.

Practice

Part C2025 Juneshow ▾
Let u(x) be the solution to the Volterra integral equation u(x)=x2+4∫0u(x) = x^{2} + 4\int_{0}ˣ (t−x)2u(t)(t - x)^{2}u(t) dt. Then which of the following statements are true?
  1. A.u(0) = 0✓ Correct
  2. B.u(2π/3)=u(2\pi/\sqrt{3}) = (1/6)(e4π/3(1/6)(e^{4\pi/\sqrt{3}} − e−2π/3)e^{-2\pi/\sqrt{3}})✓ Correct
  3. C.u(π/(23))=u(\pi/(2\sqrt{3})) = (1/6)(eπ/3(1/6)(e^{\pi/\sqrt{3}} −3- \sqrt{3} e−π/(23))e^{-\pi/(2\sqrt{3})})✓ Correct
  4. D.u(π/(23))=u(\pi/(2\sqrt{3})) = (1/6)(eπ/3(1/6)(e^{\pi/\sqrt{3}} +3+ \sqrt{3} e−π/3)e^{-\pi/\sqrt{3}})

The worked solution and the per-option analysis are in Trap Analysis.

Part C2025 Decembershow ▾
Let y(x) be the solution of the integral equation (IE) y(x) = eˣ +e+1+(1/3)∫01y(t)+ e + 1 + (1/3)\int_{0}^{1}y(t)dt, and R(x,t,1/3) be the resolvent kernel associated to IE. Then which of the following statements are true?
  1. A.R(0,1,1/3) = 3/2✓ Correct
  2. B.R(1/2,1/2,1/3) = 2/3
  3. C.y(1) = 3e+1✓ Correct
  4. D.y(1) = e+3

The worked solution and the per-option analysis are in Trap Analysis.

Part B2025 Decembershow ▾
Suppose u(x) is the solution of the integral equation u(x)=3+∫0u(x) = 3 + \int_{0}ˣ (x−t)u(t) dt. Then which of the following statements is true?
  1. A.u(π)=2eπu(\pi) = 2e^\pi.
  2. B.u′(π)=eπu'(\pi) = e^\pi.
  3. C.u(π)+u′(π)=3eπu(\pi) + u'(\pi) = 3e^\pi.✓ Correct
  4. D.u(π)−u′(π)=eπu(\pi) - u'(\pi) = e^\pi.

The worked solution and the per-option analysis are in Trap Analysis.

Part C2025 Juneshow ▾
Let f and K be such that the solution of the initial value problem y″ − 3y′ + 2y = 4sin(x), y(0) = 1, y′(0) = −2 satisfies the Volterra integral equation y(x)=f(x)+∫0y(x) = f(x) + \int_{0}ˣ K(x, t)y(t) dt. Then which of the following statements are true?
  1. A.f′(π)=3f'(\pi) = 3✓ Correct
  2. B.f(π)+f′(π)=4−πf(\pi) + f'(\pi) = 4 - \pi✓ Correct
  3. C.f(π)+f′(π)=2−πf(\pi) + f'(\pi) = 2 - \pi
  4. D.f(0) + f′(0) = −4✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part C2025 Decembershow ▾
Let λ∈R\lambda\in\mathbb{R} be such that the integral equation y(x)=λ∫y(x) = \lambda\int₋11(5_{1}^{1}(5xt3+4x2t+3^{3}+4x^{2}t+3xt)y(t)dt admits a non-trivial solution y(x) such that y(1)=5/2. Then which of the following statements are true?
  1. A.y(0)+y′(0) = 3/2✓ Correct
  2. B.y(1/2)+y′(1/2) = 7/2✓ Correct
  3. C.y(−1)+y′(−1) = −1✓ Correct
  4. D.y(1/3)+y′(1/3) = 14/9

The worked solution and the per-option analysis are in Trap Analysis.

Part C2024 Decembershow ▾
The integral equation u(x)=f(x)+(2/π)∫0πsin⁡(x−t)u(t)u(x) = f(x) + (2/\pi)\int_{0}^\pi \sin(x - t)u(t)dt has a unique solution if
  1. A.f(x) = cos x✓ Correct
  2. B.f(x) = cos 5x✓ Correct
  3. C.f(x) = sin x✓ Correct
  4. D.f(x) = sin 5x✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part C2024 Decembershow ▾
If u is the solution of the Volterra integral equation u(x)=3+sin⁡x+∫0u(x) = 3 + \sin x + \int_{0}ˣ [(3 + sin x)/(3 + sin t)]u(t)dt, then
  1. A.u(π/2)=4e(π/2)u(\pi/2) = 4e^(\pi/2)✓ Correct
  2. B.u(π)=3eπu(\pi) = 3e^\pi✓ Correct
  3. C.u(−π)=4e(−π)u(-\pi) = 4e^(-\pi)
  4. D.u(−π/2)=4eπu(-\pi/2) = 4e^\pi

The worked solution and the per-option analysis are in Trap Analysis.

Part C2024 Decembershow ▾
The integral equation u(x)=f(x)+(2/π)∫0πcos⁡(x+t)u(t)u(x) = f(x) + (2/\pi)\int_{0}^\pi \cos(x + t)u(t)dt has infinitely many solutions if
  1. A.f(x) = cos x
  2. B.f(x) = cos 5x✓ Correct
  3. C.f(x) = sin x✓ Correct
  4. D.f(x) = sin 5x✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part B2024 Juneshow ▾
Let u be the solution of the Volterra integral equation ∫0\int_{0}ᵗ [½ +sin⁡(t−τ)]u(τ)dτ=sin⁡t+ \sin(t - \tau)] u(\tau) d\tau = \sin t. Then the value of u(1) is
  1. A.0✓ Correct
  2. B.1
  3. C.2
  4. D.2e⁻1^{1}

The worked solution and the per-option analysis are in Trap Analysis.

Part C2024 Juneshow ▾
For c∈Rc \in \mathbb{R}, consider the following Fredholm integral equation y(x) = 1 + x + cx2+2∫01(1−3^{2} + 2\int_{0}^{1} (1 - 3xt)y(t)dt. Then the values of c for which the integral equation admits a solution are
  1. A.−8✓ Correct
  2. B.−6
  3. C.2
  4. D.6

The worked solution and the per-option analysis are in Trap Analysis.

Part B2023 Juneshow ▾
For the unknown y:[0,1]→Ry : [0,1] \to \mathbb{R}, consider the boundary value problem y″(x) + 2y(x) = 0 for x ∈ (0,1), y(0) = y(1) = 0. It is given that it corresponds to the integral equation y(x)=2∫01K(x,t)y(t)y(x) = 2\int_{0}^{1} K(x, t) y(t) dt. Which of the following is the kernel K(x, t)?
  1. A.K(x,t) = t(1 − x) for t < x; x(1 − t) for t > x✓ Correct
  2. B.K(x,t)=t2(1−x)K(x,t) = t^{2}(1 - x) for t<x;x2(1−t)t < x; x^{2}(1 - t) for t > x
  3. C.K(x,t)=t(1−x)K(x,t) = \sqrt{t}(1 - x) for t<x;x(1−t)t < x; \sqrt{x}(1 - t) for t > x
  4. D.K(x,t)=t3(1−x)K(x,t) = \sqrt{t^{3}}(1 - x) for t<x;x3(1−t)t < x; \sqrt{x^{3}}(1 - t) for t > x

Solution

The Green's function of −y″ with Dirichlet conditions on [0,1] is G(x,t) = t(1 − x) for t < x and x(1 − t) for t > x; then y=2∫Gyy = 2\int{}G y.

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Part B2023 Decembershow ▾
The value of λ\lambda for which the integral equation y(x)=λ∫01x2y(x) = \lambda\int_{0}^{1} x^{2} ex+te^{x+t} y(t) dt has a non-zero solution is
  1. A.4/(1+e2)4/(1 + e^{2})
  2. B.2/(1+e2)2/(1 + e^{2})
  3. C.4/(e2−1)4/(e^{2} - 1)✓ Correct
  4. D.2/(e2−1)2/(e^{2} - 1)

Solution

Separable kernel: y=cx2ey = c x^{2}eˣ with c=λc∫01t2c = \lambda{}c \int_{0}^{1} t^{2} e2te^{2t} dt =λc(e2−1)/4= \lambda{}c (e^{2} - 1)/4, so λ=4/(e2−1)\lambda = 4/(e^{2} - 1).

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Part C2023 Decembershow ▾
Let y be the solution to the Volterra integral equation y(x) = eˣ +∫0+ \int_{0}ˣ ((1+x2)/(1+t2))y(t)((1 + x^{2})/(1 + t^{2})) y(t) dt. Which of the following statements are true?
  1. A.y(1)=(1+π/4)ey(1) = (1 + \pi/4)e
  2. B.y(1)=(1+π/2)ey(1) = (1 + \pi/2)e✓ Correct
  3. C.y(3)=(1+y(\sqrt{3}) = (1 + 3π/4)e33\pi/4)e^{\sqrt{3}}
  4. D.y(3)=(1+y(\sqrt{3}) = (1 + 4π/3)e34\pi/3)e^{\sqrt{3}}✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part C2023 Decembershow ▾
Consider the Fredholm integral equation y(x)−3∫01txy(t)y(x) - 3\int_{0}^{1} t x y(t) dt = f(x), with f continuous on [0, 1]. Which of the following choices for f(x) have the property that the equation admits at least one solution?
  1. A.f(x)=x2−1/2f(x) = x^{2} - 1/2✓ Correct
  2. B.f(x) = eˣ
  3. C.f(x) = 2 − 3x✓ Correct
  4. D.f(x) = x − 1

The worked solution and the per-option analysis are in Trap Analysis.

Part Cshow ▾
Consider the Volterra equation u(x)=f(x)+λ∫0u(x) = f(x) + \lambda\int_{0}ˣ K(x, t)u(t) dt with K and f continuous on a bounded interval. Which of the following are true?
  1. A.A unique continuous solution exists for every value of λ\lambda.✓ Correct
  2. B.The Neumann (successive-approximation) series converges for every λ\lambda.✓ Correct
  3. C.The analogous Fredholm equation (fixed integration limits) is also uniquely solvable for every λ\lambda.
  4. D.If K ≡ 0, the solution is u = f.✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part Bshow ▾
The solution of the Volterra equation u(x)=x+∫0u(x) = x + \int_{0}ˣ u(t) dt is
  1. A.u(x) = eˣ − 1✓ Correct
  2. B.u(x) = eˣ
  3. C.u(x)=x+x2/2u(x) = x + x^{2}/2
  4. D.u(x) = sinh x

Solution

Differentiate: u′ = 1 + u with u(0) = 0.

Solving gives u = Ceˣ − 1 and the initial condition makes C = 1: u = eˣ − 1.

Check in the original equation: x+∫0x + \int_{0}ˣ(eᵗ − 1)dt = x + eˣ − 1 − x = eˣ − 1 ✓.

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2. Separable kernels and resolvent kernels

Read this as a chapter →

Lec-25 Calculus of Variations and Integral Equations

NPTEL · Calculus of Variations and Integral Equations

Separable (degenerate) kernels reduce the problem to linear algebra.

Separable kernels and resolvent kernels free

In plain words

If the kernel splits into a short sum of products, the whole problem collapses into a small matrix equation, and the eigenvalues are simply where a determinant vanishes.

Separable (degenerate) kernels

K(x,t)=∑i=1nK(x, t) = \sum_{i=1}^{n} ai(x)bi(t)a_{i}(x)b_{i}(t). Substituting into y=f+λ∫y = f + \lambda\intKy and setting ci=∫biyc_{i} = \int{}b_{i} y turns the problem into

(I−λA)c=d(I - \lambda{}A)c = d, where Aij=∫biajA_{ij} = \int b_{i} a_{j} and di=∫bifd_{i} = \int b_{i} f.

−λ- \lambda is an eigenvalue ⇔det⁡(I−λA)=0,i.e.1/λ\Leftrightarrow \det(I - \lambda{}A) = 0, i.e. 1/\lambda is an eigenvalue of A.

  • At most n eigenvalues for a rank-n kernel.
  • Then y=f+λ∑ciai(x)y = f + \lambda \sum c_{i} a_{i}(x).

Example. K=x2ex+tK = x^{2}e^{x+t} on [0,1]:a(x)=x2e[0,1]: a(x) = x^{2}eˣ, b(t) = eᵗ. A=∫01t2e2tA = \int_{0}^{1} t^{2}e^{2t} dt =(e2−1)/4= (e^{2} - 1)/4, so the eigenvalue is λ=4/(e2−1)\lambda = 4/(e^{2} - 1).

Neumann series and the resolvent

Iterating y=f+λ∫y = f + \lambda\intKy gives y=f+λ∫R(x,t;λ)f(t)y = f + \lambda\int{}R(x,t;\lambda)f(t)dt with

R=K1+λK2+λ2K3+⋯R = K_{1} + \lambda{}K_{2} + \lambda^{2}K_{3} + \cdots, where KnK_{n}₊1(x,t)=∫K(x,s)Kn(s,t)_{1}(x,t) = \int{}K(x,s)K_{n}(s,t)ds are the iterated kernels.

  • Converges for |λ\lambda| < 1/‖K‖ (Fredholm), and for all λ\lambda in the Volterra case.
  • For Volterra with K=1:K2=(x−t),K3=(x−t)2/2K = 1: K_{2} = (x - t), K_{3} = (x - t)^{2}/2!, so R = eλ(x−t)e^{\lambda(x-t)}.
  • For separable K, the resolvent is a rational function of λ\lambda whose poles are the eigenvalues.

Symmetric kernels

K(x,t) = K(t,x) real ⇒ eigenvalues are real, eigenfunctions for distinct eigenvalues are orthogonal, and (Hilbert–Schmidt)K(x,t)=∑φn(x)φn(t)/λn) K(x,t) = \sum \varphi_{n}(x)\varphi_{n}(t)/\lambda_{n}. This is the integral-operator analogue of the spectral theorem.

Key takeaways

  • Rank-n separable kernel ⇒ an n × n matrix problem with at most n eigenvalues.
  • Resolvent = sum of iterated kernels; always convergent for Volterra.
  • Symmetric kernels behave like symmetric matrices.

Separable kernels turn an integral equation into linear algebrainteractive

This visual is part of Trap Analysis

A degenerate kernel reduces the whole problem to a finite system — worked.

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Exam focus: Separable kernels turn integral equations into matrix problems. The resolvent kernel sums the Neumann series and gives the solution in closed form.

Practice

Part B2025 Juneshow ▾
If y(x) is the solution of the integral equation y(x)=x2+2∫01y(x) = x^{2} + 2\int_{0}^{1} xt y(t) dt, then which of the following statements is true?
  1. A.y(0) + y(1) = 1/2
  2. B.y(−1) + y(1) = 1
  3. C.y′(0) + y′(1) = 3/2
  4. D.y′(−1) + y′(1) = 3✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part C2024 Juneshow ▾
For λ∈R\lambda \in \mathbb{R} such that |λ\lambda| < 5/32, let R(x,t,λ)R(x, t, \lambda) and u denote the resolvent kernel and the solution, respectively, of the Fredholm integral equation u(x)=x+(λ/2)∫u(x) = x + (\lambda/2)\int₋22(_{2}^{2} (xt +x2t2)u(t)+ x^{2}t^{2})u(t)dt. Then which of the following statements are true?
  1. A.R(x,t,λ)=3R(x, t, \lambda) = 3xt/(3−8λ)−5x2t2/(5−32λ)/(3 - 8\lambda) - 5x^{2}t^{2}/(5 - 32\lambda)
  2. B.R(x,t,λ)=3R(x, t, \lambda) = 3xt/(3−8λ)+5x2t2/(5−32λ)/(3 - 8\lambda) + 5x^{2}t^{2}/(5 - 32\lambda)✓ Correct
  3. C.u(1)=−5/(5−32λ)u(1) = -5/(5 - 32\lambda)
  4. D.u(1)=3/(3−8λ)u(1) = 3/(3 - 8\lambda)✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part C2024 Decembershow ▾
Let R(x, t) and u(x) denote the resolvent kernel and the solution, respectively, of the Volterra integral equation u(x) = eˣ +2∫(ln⁡6)xe(2(t−x))u(t)+ 2\int_(\ln 6)^x e^(2(t-x))u(t)dt. Then which of the following statements are true?
  1. A.R(x, t) = 1✓ Correct
  2. B.R(x, t) = e^(t−x)
  3. C.u(ln 8) = 10
  4. D.u(ln 7) = 9✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part Cshow ▾
Consider y(x)=f(x)+λ∫01y(x) = f(x) + \lambda\int_{0}^{1} xt·y(t) dt, a Fredholm equation of the second kind with separable kernel K(x, t) = xt. Which of the following are true?
  1. A.The separable kernel reduces the equation to an algebraic equation for a single unknown constant.✓ Correct
  2. B.The equation has a unique solution for every λ≠3\lambda \ne 3.✓ Correct
  3. C.λ=3\lambda = 3 is an eigenvalue of the kernel: the homogeneous equation y(x)=λ∫01y(x) = \lambda\int_{0}^{1}xt·y(t) dt has a nontrivial solution exactly when λ=3\lambda = 3.✓ Correct
  4. D.The equation has a unique solution for every value of λ\lambda, including λ=3\lambda = 3.

Solution

Writing y(x)=f(x)+λy(x) = f(x) + \lambdaxC with C=∫01t⋅y(t)C = \int_{0}^{1}t\cdot{}y(t)dt reduces the equation to C(1−λ/3)=∫01C(1 - \lambda/3) = \int_{0}^{1}tf(t)dt, giving C=3∫C = 3\inttf(t)dt/(3−λ)/(3 - \lambda) — solvable and unique whenever λ≠3\lambda \ne 3 — (1)–(2). At λ=3\lambda = 3 the coefficient (3−λ)(3 - \lambda) vanishes, exactly the eigenvalue case in (3), so (4) is false: existence and uniqueness break down at λ=3\lambda = 3, per the Fredholm alternative.

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Part Cshow ▾
Which of the following are true for the Volterra equation of the second kind y(x)=f(x)+λ∫0y(x) = f(x) + \lambda\int_{0}ˣ K(x,t)y(t)dt with K continuous?
  1. A.It has a unique solution for every λ\lambda✓ Correct
  2. B.It may have eigenvalues
  3. C.The Neumann series converges for all λ\lambda✓ Correct
  4. D.It can be converted to an initial value problem when K is a polynomial in x − t✓ Correct

The worked solution and the per-option analysis are in Trap Analysis.

Part Bshow ▾
The eigenvalue λ\lambda for which y(x)=λ∫01xty(t)y(x) = \lambda\int_{0}^{1} x t y(t) dt has a non-trivial solution is
  1. A.1
  2. B.2
  3. C.3✓ Correct
  4. D.4

Solution

Put c=∫01tyc = \int_{0}^{1} t y.

Then y=λy = \lambdacx and c=λc∫01t2c = \lambda{}c\int_{0}^{1}t^{2} dt =λc/3= \lambda{}c/3, so λ=3\lambda = 3.

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Part Cshow ▾
Let K(x,t)=∑igi(x)hi(t)K(x, t) = \sum_{i} g_{i}(x)h_{i}(t) be a separable (degenerate) kernel with finitely many terms. Which of the following are true?
  1. A.The Fredholm equation with a separable kernel always reduces to a finite linear system for constants, rather than the original integral equation.✓ Correct
  2. B.The resolvent kernel of a separable kernel is itself separable.✓ Correct
  3. C.K(x, t) = sin(x + t) is not separable (degenerate).
  4. D.K(x, t) = eˣᵗ is not separable — it cannot be written as a finite sum of products g(x)h(t).✓ Correct

Solution

(1)–(2) are the standard method for degenerate kernels and a fact about the resolvent it produces. (4) eˣᵗ =∑(= \sum(xt)n/n)^{n}/n! is a genuine infinite series with no finite reduction, so it is not degenerate. (3) is false: sin(x + t) = sin x cos t + cos x sin t IS separable, with rank 2 — a kernel built from a sum of arguments is not automatically non-separable.

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