A curious connection : What's the function $f(x)$?
Clash Royale CLAN TAG#URR8PPP
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Hello I was wondering what was the function $f$ defines like this :
Let $f(x)$ a continuous and differentiable function such that :
$$f(x)=sum_k=0^inftyfracf'(k)k!(-x)^k$$
In fact can't solve it but it makes a connection between Ramanujan's Master theorem and Frullani's integral via the Fundamental theorem of calculus I explain :
We have :
$$int_0^inftyx^-s-1f(x)dx=Gamma(-s)f'(s)$$
Or :
$$int_0^inftyfracx^-s-1f(x)Gamma(-s)dx=f'(s)$$
Now we use the Fundamental theorem of calculus to get :
$$int_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(s)-f(0)$$
Now we take the limit to get :
$$lim_stoinftyint_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(infty)-f(0)$$
Wich is equal to:
$$int_0^inftyfracf(ax)-f(bx)ln(fracab)x$$
So my question is what is the function $f(x)$ , there exists a closed form to this ,is it trivial or not ?
Thanks
Ps:I know it's not very rigorous but I think it's interesting
calculus integration
 |Â
show 6 more comments
up vote
16
down vote
favorite
Hello I was wondering what was the function $f$ defines like this :
Let $f(x)$ a continuous and differentiable function such that :
$$f(x)=sum_k=0^inftyfracf'(k)k!(-x)^k$$
In fact can't solve it but it makes a connection between Ramanujan's Master theorem and Frullani's integral via the Fundamental theorem of calculus I explain :
We have :
$$int_0^inftyx^-s-1f(x)dx=Gamma(-s)f'(s)$$
Or :
$$int_0^inftyfracx^-s-1f(x)Gamma(-s)dx=f'(s)$$
Now we use the Fundamental theorem of calculus to get :
$$int_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(s)-f(0)$$
Now we take the limit to get :
$$lim_stoinftyint_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(infty)-f(0)$$
Wich is equal to:
$$int_0^inftyfracf(ax)-f(bx)ln(fracab)x$$
So my question is what is the function $f(x)$ , there exists a closed form to this ,is it trivial or not ?
Thanks
Ps:I know it's not very rigorous but I think it's interesting
calculus integration
2
Just a quick observation, but $f(x)=0$ satisfies the condition.
â Karn Watcharasupat
12 hours ago
2
@KarnWatcharasupat The set of solutions form a vector space.
â saulspatz
12 hours ago
1
If I'm not wrong (but I'm sure I am) you can differentiate the expression of $f$ to get $f'(x)=-f(x)$ which has as solution $Ce^-x$. Developing few terms you see that $C=0$ so the unique function that satisfies the definition is the constant function $0$ (this why I think I'm misunderstanding something).
â Dog_69
12 hours ago
2
@Dog_69, you might want to verify you differentiation, I don't believe $f'(x) = -f(x)$ unfortunately
â user88595
11 hours ago
2
I am right. I was wrong after all. $f'$ gives the sum $$ -sum_k=0^infty fracf'(k+1)k!(-x)^k$$ which is different from $-f$. Thanks @user88595. It was too easy to be true.
â Dog_69
11 hours ago
 |Â
show 6 more comments
up vote
16
down vote
favorite
up vote
16
down vote
favorite
Hello I was wondering what was the function $f$ defines like this :
Let $f(x)$ a continuous and differentiable function such that :
$$f(x)=sum_k=0^inftyfracf'(k)k!(-x)^k$$
In fact can't solve it but it makes a connection between Ramanujan's Master theorem and Frullani's integral via the Fundamental theorem of calculus I explain :
We have :
$$int_0^inftyx^-s-1f(x)dx=Gamma(-s)f'(s)$$
Or :
$$int_0^inftyfracx^-s-1f(x)Gamma(-s)dx=f'(s)$$
Now we use the Fundamental theorem of calculus to get :
$$int_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(s)-f(0)$$
Now we take the limit to get :
$$lim_stoinftyint_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(infty)-f(0)$$
Wich is equal to:
$$int_0^inftyfracf(ax)-f(bx)ln(fracab)x$$
So my question is what is the function $f(x)$ , there exists a closed form to this ,is it trivial or not ?
Thanks
Ps:I know it's not very rigorous but I think it's interesting
calculus integration
Hello I was wondering what was the function $f$ defines like this :
Let $f(x)$ a continuous and differentiable function such that :
$$f(x)=sum_k=0^inftyfracf'(k)k!(-x)^k$$
In fact can't solve it but it makes a connection between Ramanujan's Master theorem and Frullani's integral via the Fundamental theorem of calculus I explain :
We have :
$$int_0^inftyx^-s-1f(x)dx=Gamma(-s)f'(s)$$
Or :
$$int_0^inftyfracx^-s-1f(x)Gamma(-s)dx=f'(s)$$
Now we use the Fundamental theorem of calculus to get :
$$int_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(s)-f(0)$$
Now we take the limit to get :
$$lim_stoinftyint_0^sint_0^inftyfracx^-s-1f(x)Gamma(-s)dxds=f(infty)-f(0)$$
Wich is equal to:
$$int_0^inftyfracf(ax)-f(bx)ln(fracab)x$$
So my question is what is the function $f(x)$ , there exists a closed form to this ,is it trivial or not ?
Thanks
Ps:I know it's not very rigorous but I think it's interesting
calculus integration
asked 12 hours ago
FatsWallers
132217
132217
2
Just a quick observation, but $f(x)=0$ satisfies the condition.
â Karn Watcharasupat
12 hours ago
2
@KarnWatcharasupat The set of solutions form a vector space.
â saulspatz
12 hours ago
1
If I'm not wrong (but I'm sure I am) you can differentiate the expression of $f$ to get $f'(x)=-f(x)$ which has as solution $Ce^-x$. Developing few terms you see that $C=0$ so the unique function that satisfies the definition is the constant function $0$ (this why I think I'm misunderstanding something).
â Dog_69
12 hours ago
2
@Dog_69, you might want to verify you differentiation, I don't believe $f'(x) = -f(x)$ unfortunately
â user88595
11 hours ago
2
I am right. I was wrong after all. $f'$ gives the sum $$ -sum_k=0^infty fracf'(k+1)k!(-x)^k$$ which is different from $-f$. Thanks @user88595. It was too easy to be true.
â Dog_69
11 hours ago
 |Â
show 6 more comments
2
Just a quick observation, but $f(x)=0$ satisfies the condition.
â Karn Watcharasupat
12 hours ago
2
@KarnWatcharasupat The set of solutions form a vector space.
â saulspatz
12 hours ago
1
If I'm not wrong (but I'm sure I am) you can differentiate the expression of $f$ to get $f'(x)=-f(x)$ which has as solution $Ce^-x$. Developing few terms you see that $C=0$ so the unique function that satisfies the definition is the constant function $0$ (this why I think I'm misunderstanding something).
â Dog_69
12 hours ago
2
@Dog_69, you might want to verify you differentiation, I don't believe $f'(x) = -f(x)$ unfortunately
â user88595
11 hours ago
2
I am right. I was wrong after all. $f'$ gives the sum $$ -sum_k=0^infty fracf'(k+1)k!(-x)^k$$ which is different from $-f$. Thanks @user88595. It was too easy to be true.
â Dog_69
11 hours ago
2
2
Just a quick observation, but $f(x)=0$ satisfies the condition.
â Karn Watcharasupat
12 hours ago
Just a quick observation, but $f(x)=0$ satisfies the condition.
â Karn Watcharasupat
12 hours ago
2
2
@KarnWatcharasupat The set of solutions form a vector space.
â saulspatz
12 hours ago
@KarnWatcharasupat The set of solutions form a vector space.
â saulspatz
12 hours ago
1
1
If I'm not wrong (but I'm sure I am) you can differentiate the expression of $f$ to get $f'(x)=-f(x)$ which has as solution $Ce^-x$. Developing few terms you see that $C=0$ so the unique function that satisfies the definition is the constant function $0$ (this why I think I'm misunderstanding something).
â Dog_69
12 hours ago
If I'm not wrong (but I'm sure I am) you can differentiate the expression of $f$ to get $f'(x)=-f(x)$ which has as solution $Ce^-x$. Developing few terms you see that $C=0$ so the unique function that satisfies the definition is the constant function $0$ (this why I think I'm misunderstanding something).
â Dog_69
12 hours ago
2
2
@Dog_69, you might want to verify you differentiation, I don't believe $f'(x) = -f(x)$ unfortunately
â user88595
11 hours ago
@Dog_69, you might want to verify you differentiation, I don't believe $f'(x) = -f(x)$ unfortunately
â user88595
11 hours ago
2
2
I am right. I was wrong after all. $f'$ gives the sum $$ -sum_k=0^infty fracf'(k+1)k!(-x)^k$$ which is different from $-f$. Thanks @user88595. It was too easy to be true.
â Dog_69
11 hours ago
I am right. I was wrong after all. $f'$ gives the sum $$ -sum_k=0^infty fracf'(k+1)k!(-x)^k$$ which is different from $-f$. Thanks @user88595. It was too easy to be true.
â Dog_69
11 hours ago
 |Â
show 6 more comments
2 Answers
2
active
oldest
votes
up vote
4
down vote
Not a full answer, but a set of equations to exploit.
Let
$$
g(x) = f'(x)=sum_k=1^inftyfrack f'(k)k!(-1)^k x^k-1= sum_k=0^inftyfracg(k+1)k!(-1)^k+1 x^k
$$
But also, via Taylor expansion
$$
g(x) = sum_k=0^inftyfracg^(k)(0)k! x^k
$$
So we obtain the set of equations, for all $k=0 cdots infty$:
$$
g^(k)(0) = g(k+1)(-1)^k+1
$$
The first few are:
$$
g(0) = - g(1)\
g'(0) = g(2)\
g''(0) = - g(3)\
g^(3)(0) = g(4)\
cdots
$$
Can we proceed from here?
Let $g(x)=-f'(-x)$ instead to remove the alternating signs, and then we may use the results derived in Is there a function with the property $f(n)=f^(n)(0)$?
â Simply Beautiful Art
9 hours ago
@SimplyBeautifulArt Using your suggestion, one gets $g^(n)(0) = f'(n+1) = - g(-(n+1))$.
â Andreas
8 hours ago
Hm, you're right. Well, using the approach from the link, one can solve what you have here already I believe.
â Simply Beautiful Art
4 hours ago
add a comment |Â
up vote
1
down vote
Considering the operator
$$
calL(f) = sum_k=0^inftyfracf'(k)k!(-x)^k
$$
and choosing
$$
f(x) = e^-W(1) x
$$
with $W(cdot)$ the Lambert function, we have
$$
calL(f) =mbox $-frac1W(1)f$
$$
because
$$
f(x) = 1-x W(1)+frac 12 W(1)^2 x^2-frac 16 W(1)^3 x^3+cdots + fracW(1)^kk!(-x)^k + cdots\
fracf(x)W(1) = -1 + e^-W(1)x-frac 12e^-2W(1)x^2+frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots
$$
with
$$
W(1)^k = e^-k W(1)
$$
I hope it helps.
2
If $f(x)=e^-ex$, then $e^k neq f'(k) =-ee^-ek$.
â Rócherz
11 hours ago
What you have established, using your proposed $f(x)$, is that $ frac-1W(1)sum_k=0^inftyfracf'(k)k!(-x)^k = 1 - e^-W(1)x+frac 12e^-2W(1)x^2-frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots = f(x) $ where the last relation follows, as you write, from $W(1)^k = e^-k W(1)$. Now, the prefactor $frac-1W(1)$ unfortunately is NOT given in the original task.
â Andreas
7 hours ago
add a comment |Â
2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
4
down vote
Not a full answer, but a set of equations to exploit.
Let
$$
g(x) = f'(x)=sum_k=1^inftyfrack f'(k)k!(-1)^k x^k-1= sum_k=0^inftyfracg(k+1)k!(-1)^k+1 x^k
$$
But also, via Taylor expansion
$$
g(x) = sum_k=0^inftyfracg^(k)(0)k! x^k
$$
So we obtain the set of equations, for all $k=0 cdots infty$:
$$
g^(k)(0) = g(k+1)(-1)^k+1
$$
The first few are:
$$
g(0) = - g(1)\
g'(0) = g(2)\
g''(0) = - g(3)\
g^(3)(0) = g(4)\
cdots
$$
Can we proceed from here?
Let $g(x)=-f'(-x)$ instead to remove the alternating signs, and then we may use the results derived in Is there a function with the property $f(n)=f^(n)(0)$?
â Simply Beautiful Art
9 hours ago
@SimplyBeautifulArt Using your suggestion, one gets $g^(n)(0) = f'(n+1) = - g(-(n+1))$.
â Andreas
8 hours ago
Hm, you're right. Well, using the approach from the link, one can solve what you have here already I believe.
â Simply Beautiful Art
4 hours ago
add a comment |Â
up vote
4
down vote
Not a full answer, but a set of equations to exploit.
Let
$$
g(x) = f'(x)=sum_k=1^inftyfrack f'(k)k!(-1)^k x^k-1= sum_k=0^inftyfracg(k+1)k!(-1)^k+1 x^k
$$
But also, via Taylor expansion
$$
g(x) = sum_k=0^inftyfracg^(k)(0)k! x^k
$$
So we obtain the set of equations, for all $k=0 cdots infty$:
$$
g^(k)(0) = g(k+1)(-1)^k+1
$$
The first few are:
$$
g(0) = - g(1)\
g'(0) = g(2)\
g''(0) = - g(3)\
g^(3)(0) = g(4)\
cdots
$$
Can we proceed from here?
Let $g(x)=-f'(-x)$ instead to remove the alternating signs, and then we may use the results derived in Is there a function with the property $f(n)=f^(n)(0)$?
â Simply Beautiful Art
9 hours ago
@SimplyBeautifulArt Using your suggestion, one gets $g^(n)(0) = f'(n+1) = - g(-(n+1))$.
â Andreas
8 hours ago
Hm, you're right. Well, using the approach from the link, one can solve what you have here already I believe.
â Simply Beautiful Art
4 hours ago
add a comment |Â
up vote
4
down vote
up vote
4
down vote
Not a full answer, but a set of equations to exploit.
Let
$$
g(x) = f'(x)=sum_k=1^inftyfrack f'(k)k!(-1)^k x^k-1= sum_k=0^inftyfracg(k+1)k!(-1)^k+1 x^k
$$
But also, via Taylor expansion
$$
g(x) = sum_k=0^inftyfracg^(k)(0)k! x^k
$$
So we obtain the set of equations, for all $k=0 cdots infty$:
$$
g^(k)(0) = g(k+1)(-1)^k+1
$$
The first few are:
$$
g(0) = - g(1)\
g'(0) = g(2)\
g''(0) = - g(3)\
g^(3)(0) = g(4)\
cdots
$$
Can we proceed from here?
Not a full answer, but a set of equations to exploit.
Let
$$
g(x) = f'(x)=sum_k=1^inftyfrack f'(k)k!(-1)^k x^k-1= sum_k=0^inftyfracg(k+1)k!(-1)^k+1 x^k
$$
But also, via Taylor expansion
$$
g(x) = sum_k=0^inftyfracg^(k)(0)k! x^k
$$
So we obtain the set of equations, for all $k=0 cdots infty$:
$$
g^(k)(0) = g(k+1)(-1)^k+1
$$
The first few are:
$$
g(0) = - g(1)\
g'(0) = g(2)\
g''(0) = - g(3)\
g^(3)(0) = g(4)\
cdots
$$
Can we proceed from here?
answered 11 hours ago
Andreas
6,502834
6,502834
Let $g(x)=-f'(-x)$ instead to remove the alternating signs, and then we may use the results derived in Is there a function with the property $f(n)=f^(n)(0)$?
â Simply Beautiful Art
9 hours ago
@SimplyBeautifulArt Using your suggestion, one gets $g^(n)(0) = f'(n+1) = - g(-(n+1))$.
â Andreas
8 hours ago
Hm, you're right. Well, using the approach from the link, one can solve what you have here already I believe.
â Simply Beautiful Art
4 hours ago
add a comment |Â
Let $g(x)=-f'(-x)$ instead to remove the alternating signs, and then we may use the results derived in Is there a function with the property $f(n)=f^(n)(0)$?
â Simply Beautiful Art
9 hours ago
@SimplyBeautifulArt Using your suggestion, one gets $g^(n)(0) = f'(n+1) = - g(-(n+1))$.
â Andreas
8 hours ago
Hm, you're right. Well, using the approach from the link, one can solve what you have here already I believe.
â Simply Beautiful Art
4 hours ago
Let $g(x)=-f'(-x)$ instead to remove the alternating signs, and then we may use the results derived in Is there a function with the property $f(n)=f^(n)(0)$?
â Simply Beautiful Art
9 hours ago
Let $g(x)=-f'(-x)$ instead to remove the alternating signs, and then we may use the results derived in Is there a function with the property $f(n)=f^(n)(0)$?
â Simply Beautiful Art
9 hours ago
@SimplyBeautifulArt Using your suggestion, one gets $g^(n)(0) = f'(n+1) = - g(-(n+1))$.
â Andreas
8 hours ago
@SimplyBeautifulArt Using your suggestion, one gets $g^(n)(0) = f'(n+1) = - g(-(n+1))$.
â Andreas
8 hours ago
Hm, you're right. Well, using the approach from the link, one can solve what you have here already I believe.
â Simply Beautiful Art
4 hours ago
Hm, you're right. Well, using the approach from the link, one can solve what you have here already I believe.
â Simply Beautiful Art
4 hours ago
add a comment |Â
up vote
1
down vote
Considering the operator
$$
calL(f) = sum_k=0^inftyfracf'(k)k!(-x)^k
$$
and choosing
$$
f(x) = e^-W(1) x
$$
with $W(cdot)$ the Lambert function, we have
$$
calL(f) =mbox $-frac1W(1)f$
$$
because
$$
f(x) = 1-x W(1)+frac 12 W(1)^2 x^2-frac 16 W(1)^3 x^3+cdots + fracW(1)^kk!(-x)^k + cdots\
fracf(x)W(1) = -1 + e^-W(1)x-frac 12e^-2W(1)x^2+frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots
$$
with
$$
W(1)^k = e^-k W(1)
$$
I hope it helps.
2
If $f(x)=e^-ex$, then $e^k neq f'(k) =-ee^-ek$.
â Rócherz
11 hours ago
What you have established, using your proposed $f(x)$, is that $ frac-1W(1)sum_k=0^inftyfracf'(k)k!(-x)^k = 1 - e^-W(1)x+frac 12e^-2W(1)x^2-frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots = f(x) $ where the last relation follows, as you write, from $W(1)^k = e^-k W(1)$. Now, the prefactor $frac-1W(1)$ unfortunately is NOT given in the original task.
â Andreas
7 hours ago
add a comment |Â
up vote
1
down vote
Considering the operator
$$
calL(f) = sum_k=0^inftyfracf'(k)k!(-x)^k
$$
and choosing
$$
f(x) = e^-W(1) x
$$
with $W(cdot)$ the Lambert function, we have
$$
calL(f) =mbox $-frac1W(1)f$
$$
because
$$
f(x) = 1-x W(1)+frac 12 W(1)^2 x^2-frac 16 W(1)^3 x^3+cdots + fracW(1)^kk!(-x)^k + cdots\
fracf(x)W(1) = -1 + e^-W(1)x-frac 12e^-2W(1)x^2+frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots
$$
with
$$
W(1)^k = e^-k W(1)
$$
I hope it helps.
2
If $f(x)=e^-ex$, then $e^k neq f'(k) =-ee^-ek$.
â Rócherz
11 hours ago
What you have established, using your proposed $f(x)$, is that $ frac-1W(1)sum_k=0^inftyfracf'(k)k!(-x)^k = 1 - e^-W(1)x+frac 12e^-2W(1)x^2-frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots = f(x) $ where the last relation follows, as you write, from $W(1)^k = e^-k W(1)$. Now, the prefactor $frac-1W(1)$ unfortunately is NOT given in the original task.
â Andreas
7 hours ago
add a comment |Â
up vote
1
down vote
up vote
1
down vote
Considering the operator
$$
calL(f) = sum_k=0^inftyfracf'(k)k!(-x)^k
$$
and choosing
$$
f(x) = e^-W(1) x
$$
with $W(cdot)$ the Lambert function, we have
$$
calL(f) =mbox $-frac1W(1)f$
$$
because
$$
f(x) = 1-x W(1)+frac 12 W(1)^2 x^2-frac 16 W(1)^3 x^3+cdots + fracW(1)^kk!(-x)^k + cdots\
fracf(x)W(1) = -1 + e^-W(1)x-frac 12e^-2W(1)x^2+frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots
$$
with
$$
W(1)^k = e^-k W(1)
$$
I hope it helps.
Considering the operator
$$
calL(f) = sum_k=0^inftyfracf'(k)k!(-x)^k
$$
and choosing
$$
f(x) = e^-W(1) x
$$
with $W(cdot)$ the Lambert function, we have
$$
calL(f) =mbox $-frac1W(1)f$
$$
because
$$
f(x) = 1-x W(1)+frac 12 W(1)^2 x^2-frac 16 W(1)^3 x^3+cdots + fracW(1)^kk!(-x)^k + cdots\
fracf(x)W(1) = -1 + e^-W(1)x-frac 12e^-2W(1)x^2+frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots
$$
with
$$
W(1)^k = e^-k W(1)
$$
I hope it helps.
edited 7 hours ago
answered 11 hours ago
Cesareo
5,4592412
5,4592412
2
If $f(x)=e^-ex$, then $e^k neq f'(k) =-ee^-ek$.
â Rócherz
11 hours ago
What you have established, using your proposed $f(x)$, is that $ frac-1W(1)sum_k=0^inftyfracf'(k)k!(-x)^k = 1 - e^-W(1)x+frac 12e^-2W(1)x^2-frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots = f(x) $ where the last relation follows, as you write, from $W(1)^k = e^-k W(1)$. Now, the prefactor $frac-1W(1)$ unfortunately is NOT given in the original task.
â Andreas
7 hours ago
add a comment |Â
2
If $f(x)=e^-ex$, then $e^k neq f'(k) =-ee^-ek$.
â Rócherz
11 hours ago
What you have established, using your proposed $f(x)$, is that $ frac-1W(1)sum_k=0^inftyfracf'(k)k!(-x)^k = 1 - e^-W(1)x+frac 12e^-2W(1)x^2-frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots = f(x) $ where the last relation follows, as you write, from $W(1)^k = e^-k W(1)$. Now, the prefactor $frac-1W(1)$ unfortunately is NOT given in the original task.
â Andreas
7 hours ago
2
2
If $f(x)=e^-ex$, then $e^k neq f'(k) =-ee^-ek$.
â Rócherz
11 hours ago
If $f(x)=e^-ex$, then $e^k neq f'(k) =-ee^-ek$.
â Rócherz
11 hours ago
What you have established, using your proposed $f(x)$, is that $ frac-1W(1)sum_k=0^inftyfracf'(k)k!(-x)^k = 1 - e^-W(1)x+frac 12e^-2W(1)x^2-frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots = f(x) $ where the last relation follows, as you write, from $W(1)^k = e^-k W(1)$. Now, the prefactor $frac-1W(1)$ unfortunately is NOT given in the original task.
â Andreas
7 hours ago
What you have established, using your proposed $f(x)$, is that $ frac-1W(1)sum_k=0^inftyfracf'(k)k!(-x)^k = 1 - e^-W(1)x+frac 12e^-2W(1)x^2-frac 16 e^-3W(1)x^3+cdots + frace^-kW(1)(-x)^kk!+cdots = f(x) $ where the last relation follows, as you write, from $W(1)^k = e^-k W(1)$. Now, the prefactor $frac-1W(1)$ unfortunately is NOT given in the original task.
â Andreas
7 hours ago
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2
Just a quick observation, but $f(x)=0$ satisfies the condition.
â Karn Watcharasupat
12 hours ago
2
@KarnWatcharasupat The set of solutions form a vector space.
â saulspatz
12 hours ago
1
If I'm not wrong (but I'm sure I am) you can differentiate the expression of $f$ to get $f'(x)=-f(x)$ which has as solution $Ce^-x$. Developing few terms you see that $C=0$ so the unique function that satisfies the definition is the constant function $0$ (this why I think I'm misunderstanding something).
â Dog_69
12 hours ago
2
@Dog_69, you might want to verify you differentiation, I don't believe $f'(x) = -f(x)$ unfortunately
â user88595
11 hours ago
2
I am right. I was wrong after all. $f'$ gives the sum $$ -sum_k=0^infty fracf'(k+1)k!(-x)^k$$ which is different from $-f$. Thanks @user88595. It was too easy to be true.
â Dog_69
11 hours ago