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admin Administator 4 posts

edited 5 years ago

Since we’re stuck here in quarantine, it would be a good idea to have a place to discuss the subject of this course online.

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Equations are pretty easy to type. If you type

The $N$-point tree-level S-Matrix is
$$
  S_N(p_1,\dots,p_N) = \frac{8\pi i}{\alpha'} g_s^{2(N-2)}
    \int |z_{1 2}|^2 |z_{1 3}|^2 |z_{2 3}|^2\langle O_1(z_1,\overline{z}_1)
    \dots O_N(z_N,\overline{z}_N)\rangle d^2 z_4\dots d^2 z_N.
$$
where the $O_i$ are $h=\tilde{h}=1$ conformal primaries in the theory of 26 free scalars.

You get

The NN-point tree-level S-Matrix is

S N(p 1,,p N)=8πiαg s 2(N2)|z 12| 2|z 13| 2|z 23| 2O 1(z 1,z¯ 1)O N(z N,z¯ N)d 2z 4d 2z N. S_N(p_1,\dots,p_N) = \frac{8\pi i}{\alpha'} g_s^{2(N-2)} \int |z_{1 2}|^2 |z_{1 3}|^2 |z_{2 3}|^2\langle O_1(z_1,\overline{z}_1) \dots O_N(z_N,\overline{z}_N)\rangle d^2 z_4\dots d^2 z_N.

where the O iO_i are h=h˜=1h=\tilde{h}=1 conformal primaries in the theory of 26 free scalars.

and

The 4-point tachyon amplitude is
\[
   S_4(p_1,p_2,p_3,p_4) = \frac{8\pi i}{\alpha'} g_s^4 (2\pi)^{26}
     \delta^{(26)}\bigl(\sum p_i\bigr)2\pi \frac{\Gamma\bigl(-\tfrac{\alpha' s}{4}-1\bigr)
       \Gamma\bigl(-\tfrac{\alpha' t}{4}-1\bigr)\Gamma\bigl(-\tfrac{\alpha' u}{4}-1\bigr)
       }{\Gamma\bigl(\tfrac{\alpha' u}{4}+2\bigr)\Gamma\bigl(\tfrac{\alpha' t}{4}+2\bigr)
      \Gamma\bigl(\tfrac{\alpha' s}{4}+2\bigr)}
\]

produces

The 4-point tachyon amplitude is

(1)S 4(p 1,p 2,p 3,p 4)=8πiαg s 4(2π) 26δ (26)(p i)2πΓ(αs41)Γ(αt41)Γ(αu41)Γ(αu4+2)Γ(αt4+2)Γ(αs4+2) S_4(p_1,p_2,p_3,p_4) = \frac{8\pi i}{\alpha'} g_s^4 (2\pi)^{26} \delta^{(26)}\bigl(\sum p_i\bigr)2\pi \frac{\Gamma\bigl(-\tfrac{\alpha' s}{4}-1\bigr)\Gamma\bigl(-\tfrac{\alpha' t}{4}-1\bigr)\Gamma\bigl(-\tfrac{\alpha' u}{4}-1\bigr)}{\Gamma\bigl(\tfrac{\alpha' u}{4}+2\bigr)\Gamma\bigl(\tfrac{\alpha' t}{4}+2\bigr)\Gamma\bigl(\tfrac{\alpha' s}{4}+2\bigr)}

The full equation syntax may be a little daunting, but you probably won’t need much more than the above. For the rest, there’s Markdown.

Oh, and you can draw pictures, using the built-in drawing tool.

Layer 1 p 1 p_1 p 2 p_2 p 3 p_3 p 4 p_4 s 4 n α s\to \frac{4n}{\alpha'} p 1 p_1 p 2 p_2 p 3 p_3 p 4 p_4 G ( p 2 ) G(p^2) = d 26 p ( 2 π ) 26 ={\int\frac{d^{26}p}{(2\pi)^{26}}}

(Just click on the “Create SVG Graphic”) button.

 
Charlie 1 post

This is cool. Once I draw a picture in the SVG editor, how do I get it to be part of a post?

 
admin Administator 4 posts

When you choose “SVG-Edit → Save Image” in the SVG Edit window, it will save the SVG code back to your post. When you’re done with that, just “Save reply” and the SVG will be magically-rendered.

You can also create Tikzpictures:

\ begin{tikzpicture}[every tqft/.style={fill=orange,fill opacity=0.25},
tqft/every boundary component/.style={fill=yellow,fill opacity=.5},
tqft/every upper boundary component/.style={draw,thin,blue},
tqft/every lower boundary component/.style={draw,dashed,thin,blue}]
\usetikzlibrary{tqft}
\begin{scope}[tqft/every incoming boundary component/.style={fill=green, fill opacity= .25}]
\pic[tqft/pair of pants,draw,name=a,at={(0,0)}];
\pic[tqft/reverse pair of pants,draw,anchor=incoming boundary 2,name=e,at={(8,0)}];
\end{scope}
\begin{scope}[tqft/every outgoing boundary component/.style={draw,thin,blue,fill=yellow}]
\pic[tqft/reverse pair of pants,draw,anchor=incoming boundary 1,name=b,at=(a-outgoing boundary 2)];
\end{scope}
\begin{scope}[tqft/every incoming boundary component/.style={fill=green, fill opacity= .25}]
\pic[tqft/cylinder,draw,anchor=outgoing boundary 1,name=d,at=(b-incoming boundary 2)];
\end{scope}
\path (b-incoming boundary 2) ++(1.5,0) node[font=\Huge] {\(=\)};
\begin{scope}[tqft/every outgoing boundary component/.style={draw,thin,blue,fill=yellow}]
\pic[tqft/cylinder,draw,anchor=incoming boundary 1,name=c,at=(a-outgoing boundary 1)];
\pic[tqft/pair of pants,draw,anchor=incoming boundary 1,name=f,at=(e-outgoing boundary 1)];
\end{scope}
\end{tikzpicture}

produces

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