Inline Feynman diagrams, Feynman diagrams in equations, very small Feynman diagrams












12















I'd like to typeset equations like:
Inline Feynman diagrams 1Inline Feynman diagrams 2



I have tried this with the tikz-feynman library, but the diagrams generated by it are just way too large, even with the small option (and also just look awkward). Optimally, I want to type simple diagrams even inline with the text, so that I can avoid awkwardly describing the diagram or using a lot of space and breaking the flow of the document to display the diagram.










share|improve this question


















  • 1





    Welcome to TeX.SE. I like very much your question. Good LaTeX.

    – Sebastiano
    Feb 23 at 10:44






  • 1





    Using normal inline TikZ by tikz may be a solution.

    – JouleV
    Feb 23 at 10:55
















12















I'd like to typeset equations like:
Inline Feynman diagrams 1Inline Feynman diagrams 2



I have tried this with the tikz-feynman library, but the diagrams generated by it are just way too large, even with the small option (and also just look awkward). Optimally, I want to type simple diagrams even inline with the text, so that I can avoid awkwardly describing the diagram or using a lot of space and breaking the flow of the document to display the diagram.










share|improve this question


















  • 1





    Welcome to TeX.SE. I like very much your question. Good LaTeX.

    – Sebastiano
    Feb 23 at 10:44






  • 1





    Using normal inline TikZ by tikz may be a solution.

    – JouleV
    Feb 23 at 10:55














12












12








12


3






I'd like to typeset equations like:
Inline Feynman diagrams 1Inline Feynman diagrams 2



I have tried this with the tikz-feynman library, but the diagrams generated by it are just way too large, even with the small option (and also just look awkward). Optimally, I want to type simple diagrams even inline with the text, so that I can avoid awkwardly describing the diagram or using a lot of space and breaking the flow of the document to display the diagram.










share|improve this question














I'd like to typeset equations like:
Inline Feynman diagrams 1Inline Feynman diagrams 2



I have tried this with the tikz-feynman library, but the diagrams generated by it are just way too large, even with the small option (and also just look awkward). Optimally, I want to type simple diagrams even inline with the text, so that I can avoid awkwardly describing the diagram or using a lot of space and breaking the flow of the document to display the diagram.







inline feynman






share|improve this question













share|improve this question











share|improve this question




share|improve this question










asked Feb 23 at 10:40









LeonardLeonard

634




634








  • 1





    Welcome to TeX.SE. I like very much your question. Good LaTeX.

    – Sebastiano
    Feb 23 at 10:44






  • 1





    Using normal inline TikZ by tikz may be a solution.

    – JouleV
    Feb 23 at 10:55














  • 1





    Welcome to TeX.SE. I like very much your question. Good LaTeX.

    – Sebastiano
    Feb 23 at 10:44






  • 1





    Using normal inline TikZ by tikz may be a solution.

    – JouleV
    Feb 23 at 10:55








1




1





Welcome to TeX.SE. I like very much your question. Good LaTeX.

– Sebastiano
Feb 23 at 10:44





Welcome to TeX.SE. I like very much your question. Good LaTeX.

– Sebastiano
Feb 23 at 10:44




1




1





Using normal inline TikZ by tikz may be a solution.

– JouleV
Feb 23 at 10:55





Using normal inline TikZ by tikz may be a solution.

– JouleV
Feb 23 at 10:55










1 Answer
1






active

oldest

votes


















15














AFAIK you do not get bent arrows with tikz-feynman. And since you seem not to need the graph drawing algorithms (and since they cannot be uploaded to the arXv), you may just work with plain TikZ.



documentclass[fleqn]{article}
usepackage{amsmath}
usepackage{mathrsfs}
usepackage{tikz}
usetikzlibrary{arrows.meta,bending,decorations.markings}
% from https://tex.stackexchange.com/a/430239/121799
tikzset{% inspired by https://tex.stackexchange.com/a/316050/121799
arc arrow/.style args={%
to pos #1 with length #2}{
decoration={
markings,
mark=at position 0 with {pgfextra{%
pgfmathsetmacro{tmpArrowTime}{#2/(pgfdecoratedpathlength)}
xdeftmpArrowTime{tmpArrowTime}}},
mark=at position {#1-tmpArrowTime} with {coordinate(@1);},
mark=at position {#1-2*tmpArrowTime/3} with {coordinate(@2);},
mark=at position {#1-tmpArrowTime/3} with {coordinate(@3);},
mark=at position {#1} with {coordinate(@4);
draw[-{Triangle[length=#2,bend]}]
(@1) .. controls (@2) and (@3) .. (@4);},
},
postaction=decorate,
},
fermion arc arrow/.style={arc arrow=to pos #1 with length 2.5mm},
Vertex/.style={fill,circle,inner sep=1.5pt},
insert vertex/.style={decoration={
markings,
mark=at position #1 with {node[Vertex]{};},
},
postaction=decorate}
}
DeclareMathOperator{tr}{tr}
begin{document}

[mathscr{P}(varphi)=-sumlimits_{n=1}^inftytrleft(Delta L_{12}right)^n
=vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex=0,fermion arc arrow={0.55}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+frac{1}{2}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,0.5}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.3,0.8}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}
+frac{1}{3}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,1/3,2/3}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.21,0.55,0.88}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+dots;.
]

[
G(x_1,dots x_n)=sumlimits_{m=0}^inftyfrac{1}{m!}
begin{tikzpicture}[baseline={(X.base)}]
node[circle,draw,thick,inner sep=2pt] (X) at (0,0) {$n+m$};
foreach X in {60,90,120}
{draw[thick] (X:0.6) -- (X:0.9) node[Vertex]{};}
foreach X in {-60,-80,-100,-120}
{draw[thick] (X:0.6) -- (X:0.9);}
node[rotate=-30,overlay] at (-120:1.1){$x_1$};
node[rotate=30,overlay] at (-60:1.1){$x_n$};
node at (-90:1.1){$cdots$};
end{tikzpicture}
]
end{document}


enter image description here






share|improve this answer


























  • Excuse me very much for this opinion. Can you reduce the size of the three circles? Perhaps the image of the series is more beautiful to see. PS: But what is the matter of this argument in Physics?

    – Sebastiano
    Feb 23 at 22:11








  • 1





    @Sebastiano You can control the appearance by adjusting Vertex/.style={fill,circle,inner sep=1.5pt},. I do not know what this diagram is. If the propagators were dashed, there would be a resemblance to the loops that one has to compute for the Coleman-Weinberg potential.

    – marmot
    Feb 23 at 22:15











  • I like very much your work. I not known the Coleman-Weinberg potential. Thank you very much. It will be between my favorities.

    – Sebastiano
    Feb 23 at 22:17








  • 1





    @Sebastiano To the best of my knowledge the term "dimensional transmutation" has been coined in the paper by Coleman and (Eric) Weinberg. It is a rather important observation. Whether or not the above has anything to do with it I do not know.

    – marmot
    Feb 23 at 22:22






  • 1





    @Sebastiano The second equation is just expressing the greenfunctions of a QFT in terms of a sum over all diagrams. The first is an intermediate step in a proof about the signs of feynman diagrams with fermionic fields. Both are taken from the excellent book "Functional methods in quantum field theory and statistical physics" by Vasiliev.

    – Leonard
    Feb 24 at 13:03











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1 Answer
1






active

oldest

votes








1 Answer
1






active

oldest

votes









active

oldest

votes






active

oldest

votes









15














AFAIK you do not get bent arrows with tikz-feynman. And since you seem not to need the graph drawing algorithms (and since they cannot be uploaded to the arXv), you may just work with plain TikZ.



documentclass[fleqn]{article}
usepackage{amsmath}
usepackage{mathrsfs}
usepackage{tikz}
usetikzlibrary{arrows.meta,bending,decorations.markings}
% from https://tex.stackexchange.com/a/430239/121799
tikzset{% inspired by https://tex.stackexchange.com/a/316050/121799
arc arrow/.style args={%
to pos #1 with length #2}{
decoration={
markings,
mark=at position 0 with {pgfextra{%
pgfmathsetmacro{tmpArrowTime}{#2/(pgfdecoratedpathlength)}
xdeftmpArrowTime{tmpArrowTime}}},
mark=at position {#1-tmpArrowTime} with {coordinate(@1);},
mark=at position {#1-2*tmpArrowTime/3} with {coordinate(@2);},
mark=at position {#1-tmpArrowTime/3} with {coordinate(@3);},
mark=at position {#1} with {coordinate(@4);
draw[-{Triangle[length=#2,bend]}]
(@1) .. controls (@2) and (@3) .. (@4);},
},
postaction=decorate,
},
fermion arc arrow/.style={arc arrow=to pos #1 with length 2.5mm},
Vertex/.style={fill,circle,inner sep=1.5pt},
insert vertex/.style={decoration={
markings,
mark=at position #1 with {node[Vertex]{};},
},
postaction=decorate}
}
DeclareMathOperator{tr}{tr}
begin{document}

[mathscr{P}(varphi)=-sumlimits_{n=1}^inftytrleft(Delta L_{12}right)^n
=vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex=0,fermion arc arrow={0.55}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+frac{1}{2}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,0.5}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.3,0.8}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}
+frac{1}{3}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,1/3,2/3}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.21,0.55,0.88}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+dots;.
]

[
G(x_1,dots x_n)=sumlimits_{m=0}^inftyfrac{1}{m!}
begin{tikzpicture}[baseline={(X.base)}]
node[circle,draw,thick,inner sep=2pt] (X) at (0,0) {$n+m$};
foreach X in {60,90,120}
{draw[thick] (X:0.6) -- (X:0.9) node[Vertex]{};}
foreach X in {-60,-80,-100,-120}
{draw[thick] (X:0.6) -- (X:0.9);}
node[rotate=-30,overlay] at (-120:1.1){$x_1$};
node[rotate=30,overlay] at (-60:1.1){$x_n$};
node at (-90:1.1){$cdots$};
end{tikzpicture}
]
end{document}


enter image description here






share|improve this answer


























  • Excuse me very much for this opinion. Can you reduce the size of the three circles? Perhaps the image of the series is more beautiful to see. PS: But what is the matter of this argument in Physics?

    – Sebastiano
    Feb 23 at 22:11








  • 1





    @Sebastiano You can control the appearance by adjusting Vertex/.style={fill,circle,inner sep=1.5pt},. I do not know what this diagram is. If the propagators were dashed, there would be a resemblance to the loops that one has to compute for the Coleman-Weinberg potential.

    – marmot
    Feb 23 at 22:15











  • I like very much your work. I not known the Coleman-Weinberg potential. Thank you very much. It will be between my favorities.

    – Sebastiano
    Feb 23 at 22:17








  • 1





    @Sebastiano To the best of my knowledge the term "dimensional transmutation" has been coined in the paper by Coleman and (Eric) Weinberg. It is a rather important observation. Whether or not the above has anything to do with it I do not know.

    – marmot
    Feb 23 at 22:22






  • 1





    @Sebastiano The second equation is just expressing the greenfunctions of a QFT in terms of a sum over all diagrams. The first is an intermediate step in a proof about the signs of feynman diagrams with fermionic fields. Both are taken from the excellent book "Functional methods in quantum field theory and statistical physics" by Vasiliev.

    – Leonard
    Feb 24 at 13:03
















15














AFAIK you do not get bent arrows with tikz-feynman. And since you seem not to need the graph drawing algorithms (and since they cannot be uploaded to the arXv), you may just work with plain TikZ.



documentclass[fleqn]{article}
usepackage{amsmath}
usepackage{mathrsfs}
usepackage{tikz}
usetikzlibrary{arrows.meta,bending,decorations.markings}
% from https://tex.stackexchange.com/a/430239/121799
tikzset{% inspired by https://tex.stackexchange.com/a/316050/121799
arc arrow/.style args={%
to pos #1 with length #2}{
decoration={
markings,
mark=at position 0 with {pgfextra{%
pgfmathsetmacro{tmpArrowTime}{#2/(pgfdecoratedpathlength)}
xdeftmpArrowTime{tmpArrowTime}}},
mark=at position {#1-tmpArrowTime} with {coordinate(@1);},
mark=at position {#1-2*tmpArrowTime/3} with {coordinate(@2);},
mark=at position {#1-tmpArrowTime/3} with {coordinate(@3);},
mark=at position {#1} with {coordinate(@4);
draw[-{Triangle[length=#2,bend]}]
(@1) .. controls (@2) and (@3) .. (@4);},
},
postaction=decorate,
},
fermion arc arrow/.style={arc arrow=to pos #1 with length 2.5mm},
Vertex/.style={fill,circle,inner sep=1.5pt},
insert vertex/.style={decoration={
markings,
mark=at position #1 with {node[Vertex]{};},
},
postaction=decorate}
}
DeclareMathOperator{tr}{tr}
begin{document}

[mathscr{P}(varphi)=-sumlimits_{n=1}^inftytrleft(Delta L_{12}right)^n
=vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex=0,fermion arc arrow={0.55}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+frac{1}{2}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,0.5}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.3,0.8}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}
+frac{1}{3}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,1/3,2/3}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.21,0.55,0.88}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+dots;.
]

[
G(x_1,dots x_n)=sumlimits_{m=0}^inftyfrac{1}{m!}
begin{tikzpicture}[baseline={(X.base)}]
node[circle,draw,thick,inner sep=2pt] (X) at (0,0) {$n+m$};
foreach X in {60,90,120}
{draw[thick] (X:0.6) -- (X:0.9) node[Vertex]{};}
foreach X in {-60,-80,-100,-120}
{draw[thick] (X:0.6) -- (X:0.9);}
node[rotate=-30,overlay] at (-120:1.1){$x_1$};
node[rotate=30,overlay] at (-60:1.1){$x_n$};
node at (-90:1.1){$cdots$};
end{tikzpicture}
]
end{document}


enter image description here






share|improve this answer


























  • Excuse me very much for this opinion. Can you reduce the size of the three circles? Perhaps the image of the series is more beautiful to see. PS: But what is the matter of this argument in Physics?

    – Sebastiano
    Feb 23 at 22:11








  • 1





    @Sebastiano You can control the appearance by adjusting Vertex/.style={fill,circle,inner sep=1.5pt},. I do not know what this diagram is. If the propagators were dashed, there would be a resemblance to the loops that one has to compute for the Coleman-Weinberg potential.

    – marmot
    Feb 23 at 22:15











  • I like very much your work. I not known the Coleman-Weinberg potential. Thank you very much. It will be between my favorities.

    – Sebastiano
    Feb 23 at 22:17








  • 1





    @Sebastiano To the best of my knowledge the term "dimensional transmutation" has been coined in the paper by Coleman and (Eric) Weinberg. It is a rather important observation. Whether or not the above has anything to do with it I do not know.

    – marmot
    Feb 23 at 22:22






  • 1





    @Sebastiano The second equation is just expressing the greenfunctions of a QFT in terms of a sum over all diagrams. The first is an intermediate step in a proof about the signs of feynman diagrams with fermionic fields. Both are taken from the excellent book "Functional methods in quantum field theory and statistical physics" by Vasiliev.

    – Leonard
    Feb 24 at 13:03














15












15








15







AFAIK you do not get bent arrows with tikz-feynman. And since you seem not to need the graph drawing algorithms (and since they cannot be uploaded to the arXv), you may just work with plain TikZ.



documentclass[fleqn]{article}
usepackage{amsmath}
usepackage{mathrsfs}
usepackage{tikz}
usetikzlibrary{arrows.meta,bending,decorations.markings}
% from https://tex.stackexchange.com/a/430239/121799
tikzset{% inspired by https://tex.stackexchange.com/a/316050/121799
arc arrow/.style args={%
to pos #1 with length #2}{
decoration={
markings,
mark=at position 0 with {pgfextra{%
pgfmathsetmacro{tmpArrowTime}{#2/(pgfdecoratedpathlength)}
xdeftmpArrowTime{tmpArrowTime}}},
mark=at position {#1-tmpArrowTime} with {coordinate(@1);},
mark=at position {#1-2*tmpArrowTime/3} with {coordinate(@2);},
mark=at position {#1-tmpArrowTime/3} with {coordinate(@3);},
mark=at position {#1} with {coordinate(@4);
draw[-{Triangle[length=#2,bend]}]
(@1) .. controls (@2) and (@3) .. (@4);},
},
postaction=decorate,
},
fermion arc arrow/.style={arc arrow=to pos #1 with length 2.5mm},
Vertex/.style={fill,circle,inner sep=1.5pt},
insert vertex/.style={decoration={
markings,
mark=at position #1 with {node[Vertex]{};},
},
postaction=decorate}
}
DeclareMathOperator{tr}{tr}
begin{document}

[mathscr{P}(varphi)=-sumlimits_{n=1}^inftytrleft(Delta L_{12}right)^n
=vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex=0,fermion arc arrow={0.55}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+frac{1}{2}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,0.5}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.3,0.8}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}
+frac{1}{3}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,1/3,2/3}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.21,0.55,0.88}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+dots;.
]

[
G(x_1,dots x_n)=sumlimits_{m=0}^inftyfrac{1}{m!}
begin{tikzpicture}[baseline={(X.base)}]
node[circle,draw,thick,inner sep=2pt] (X) at (0,0) {$n+m$};
foreach X in {60,90,120}
{draw[thick] (X:0.6) -- (X:0.9) node[Vertex]{};}
foreach X in {-60,-80,-100,-120}
{draw[thick] (X:0.6) -- (X:0.9);}
node[rotate=-30,overlay] at (-120:1.1){$x_1$};
node[rotate=30,overlay] at (-60:1.1){$x_n$};
node at (-90:1.1){$cdots$};
end{tikzpicture}
]
end{document}


enter image description here






share|improve this answer















AFAIK you do not get bent arrows with tikz-feynman. And since you seem not to need the graph drawing algorithms (and since they cannot be uploaded to the arXv), you may just work with plain TikZ.



documentclass[fleqn]{article}
usepackage{amsmath}
usepackage{mathrsfs}
usepackage{tikz}
usetikzlibrary{arrows.meta,bending,decorations.markings}
% from https://tex.stackexchange.com/a/430239/121799
tikzset{% inspired by https://tex.stackexchange.com/a/316050/121799
arc arrow/.style args={%
to pos #1 with length #2}{
decoration={
markings,
mark=at position 0 with {pgfextra{%
pgfmathsetmacro{tmpArrowTime}{#2/(pgfdecoratedpathlength)}
xdeftmpArrowTime{tmpArrowTime}}},
mark=at position {#1-tmpArrowTime} with {coordinate(@1);},
mark=at position {#1-2*tmpArrowTime/3} with {coordinate(@2);},
mark=at position {#1-tmpArrowTime/3} with {coordinate(@3);},
mark=at position {#1} with {coordinate(@4);
draw[-{Triangle[length=#2,bend]}]
(@1) .. controls (@2) and (@3) .. (@4);},
},
postaction=decorate,
},
fermion arc arrow/.style={arc arrow=to pos #1 with length 2.5mm},
Vertex/.style={fill,circle,inner sep=1.5pt},
insert vertex/.style={decoration={
markings,
mark=at position #1 with {node[Vertex]{};},
},
postaction=decorate}
}
DeclareMathOperator{tr}{tr}
begin{document}

[mathscr{P}(varphi)=-sumlimits_{n=1}^inftytrleft(Delta L_{12}right)^n
=vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex=0,fermion arc arrow={0.55}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+frac{1}{2}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,0.5}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.3,0.8}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}
+frac{1}{3}
vcenter{hbox{begin{tikzpicture}
draw[thick,insert vertex/.list={0,1/3,2/3}](0,0) arc(270:-90:0.6);
draw[fermion arc arrow/.list={0.21,0.55,0.88}] (0,0) arc(270:-90:0.6);
end{tikzpicture}}}+dots;.
]

[
G(x_1,dots x_n)=sumlimits_{m=0}^inftyfrac{1}{m!}
begin{tikzpicture}[baseline={(X.base)}]
node[circle,draw,thick,inner sep=2pt] (X) at (0,0) {$n+m$};
foreach X in {60,90,120}
{draw[thick] (X:0.6) -- (X:0.9) node[Vertex]{};}
foreach X in {-60,-80,-100,-120}
{draw[thick] (X:0.6) -- (X:0.9);}
node[rotate=-30,overlay] at (-120:1.1){$x_1$};
node[rotate=30,overlay] at (-60:1.1){$x_n$};
node at (-90:1.1){$cdots$};
end{tikzpicture}
]
end{document}


enter image description here







share|improve this answer














share|improve this answer



share|improve this answer








edited Feb 23 at 15:27

























answered Feb 23 at 13:11









marmotmarmot

112k5143268




112k5143268













  • Excuse me very much for this opinion. Can you reduce the size of the three circles? Perhaps the image of the series is more beautiful to see. PS: But what is the matter of this argument in Physics?

    – Sebastiano
    Feb 23 at 22:11








  • 1





    @Sebastiano You can control the appearance by adjusting Vertex/.style={fill,circle,inner sep=1.5pt},. I do not know what this diagram is. If the propagators were dashed, there would be a resemblance to the loops that one has to compute for the Coleman-Weinberg potential.

    – marmot
    Feb 23 at 22:15











  • I like very much your work. I not known the Coleman-Weinberg potential. Thank you very much. It will be between my favorities.

    – Sebastiano
    Feb 23 at 22:17








  • 1





    @Sebastiano To the best of my knowledge the term "dimensional transmutation" has been coined in the paper by Coleman and (Eric) Weinberg. It is a rather important observation. Whether or not the above has anything to do with it I do not know.

    – marmot
    Feb 23 at 22:22






  • 1





    @Sebastiano The second equation is just expressing the greenfunctions of a QFT in terms of a sum over all diagrams. The first is an intermediate step in a proof about the signs of feynman diagrams with fermionic fields. Both are taken from the excellent book "Functional methods in quantum field theory and statistical physics" by Vasiliev.

    – Leonard
    Feb 24 at 13:03



















  • Excuse me very much for this opinion. Can you reduce the size of the three circles? Perhaps the image of the series is more beautiful to see. PS: But what is the matter of this argument in Physics?

    – Sebastiano
    Feb 23 at 22:11








  • 1





    @Sebastiano You can control the appearance by adjusting Vertex/.style={fill,circle,inner sep=1.5pt},. I do not know what this diagram is. If the propagators were dashed, there would be a resemblance to the loops that one has to compute for the Coleman-Weinberg potential.

    – marmot
    Feb 23 at 22:15











  • I like very much your work. I not known the Coleman-Weinberg potential. Thank you very much. It will be between my favorities.

    – Sebastiano
    Feb 23 at 22:17








  • 1





    @Sebastiano To the best of my knowledge the term "dimensional transmutation" has been coined in the paper by Coleman and (Eric) Weinberg. It is a rather important observation. Whether or not the above has anything to do with it I do not know.

    – marmot
    Feb 23 at 22:22






  • 1





    @Sebastiano The second equation is just expressing the greenfunctions of a QFT in terms of a sum over all diagrams. The first is an intermediate step in a proof about the signs of feynman diagrams with fermionic fields. Both are taken from the excellent book "Functional methods in quantum field theory and statistical physics" by Vasiliev.

    – Leonard
    Feb 24 at 13:03

















Excuse me very much for this opinion. Can you reduce the size of the three circles? Perhaps the image of the series is more beautiful to see. PS: But what is the matter of this argument in Physics?

– Sebastiano
Feb 23 at 22:11







Excuse me very much for this opinion. Can you reduce the size of the three circles? Perhaps the image of the series is more beautiful to see. PS: But what is the matter of this argument in Physics?

– Sebastiano
Feb 23 at 22:11






1




1





@Sebastiano You can control the appearance by adjusting Vertex/.style={fill,circle,inner sep=1.5pt},. I do not know what this diagram is. If the propagators were dashed, there would be a resemblance to the loops that one has to compute for the Coleman-Weinberg potential.

– marmot
Feb 23 at 22:15





@Sebastiano You can control the appearance by adjusting Vertex/.style={fill,circle,inner sep=1.5pt},. I do not know what this diagram is. If the propagators were dashed, there would be a resemblance to the loops that one has to compute for the Coleman-Weinberg potential.

– marmot
Feb 23 at 22:15













I like very much your work. I not known the Coleman-Weinberg potential. Thank you very much. It will be between my favorities.

– Sebastiano
Feb 23 at 22:17







I like very much your work. I not known the Coleman-Weinberg potential. Thank you very much. It will be between my favorities.

– Sebastiano
Feb 23 at 22:17






1




1





@Sebastiano To the best of my knowledge the term "dimensional transmutation" has been coined in the paper by Coleman and (Eric) Weinberg. It is a rather important observation. Whether or not the above has anything to do with it I do not know.

– marmot
Feb 23 at 22:22





@Sebastiano To the best of my knowledge the term "dimensional transmutation" has been coined in the paper by Coleman and (Eric) Weinberg. It is a rather important observation. Whether or not the above has anything to do with it I do not know.

– marmot
Feb 23 at 22:22




1




1





@Sebastiano The second equation is just expressing the greenfunctions of a QFT in terms of a sum over all diagrams. The first is an intermediate step in a proof about the signs of feynman diagrams with fermionic fields. Both are taken from the excellent book "Functional methods in quantum field theory and statistical physics" by Vasiliev.

– Leonard
Feb 24 at 13:03





@Sebastiano The second equation is just expressing the greenfunctions of a QFT in terms of a sum over all diagrams. The first is an intermediate step in a proof about the signs of feynman diagrams with fermionic fields. Both are taken from the excellent book "Functional methods in quantum field theory and statistical physics" by Vasiliev.

– Leonard
Feb 24 at 13:03


















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