Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 3403 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{3}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6523 | 0.8133 | 0.8021 | [X:[1.6162], M:[0.727, 0.8081, 0.3838, 1.1513, 0.8487, 0.8081], q:[0.869, 0.4041], qb:[0.7472, 0.4446], phi:[0.3838]] | [X:[[4]], M:[[-18], [2], [-4], [-12], [12], [2]], q:[[17], [1]], qb:[[-13], [11]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{5}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{2}^{2}$ | 0 | t^2.181 + t^2.303 + 2*t^2.424 + t^2.546 + t^3.454 + t^3.697 + t^3.819 + t^3.941 + t^4.362 + t^4.483 + 3*t^4.605 + 3*t^4.727 + 5*t^4.849 + 2*t^4.97 + t^5.092 + t^5.635 + t^5.878 + 2*t^6.122 + 3*t^6.243 + 3*t^6.365 + t^6.487 + t^6.543 + t^6.664 + 3*t^6.786 + 4*t^6.908 + 5*t^7.03 + 5*t^7.151 + 6*t^7.273 + 3*t^7.395 + t^7.517 + 2*t^7.638 + t^7.76 + t^7.816 + t^7.882 + t^8.059 - 2*t^8.181 - 4*t^8.424 + 2*t^8.546 + 4*t^8.668 + t^8.723 + 6*t^8.79 + t^8.845 + 3*t^8.911 + 3*t^8.967 - t^4.151/y - t^6.332/y - t^6.454/y - (2*t^6.576)/y + t^7.483/y + (2*t^7.605)/y + (5*t^7.727)/y + (3*t^7.849)/y + (3*t^7.97)/y - t^8.513/y - (2*t^8.757)/y + t^8.878/y - t^4.151*y - t^6.332*y - t^6.454*y - 2*t^6.576*y + t^7.483*y + 2*t^7.605*y + 5*t^7.727*y + 3*t^7.849*y + 3*t^7.97*y - t^8.513*y - 2*t^8.757*y + t^8.878*y | t^2.181/g1^18 + t^2.303/g1^8 + 2*g1^2*t^2.424 + g1^12*t^2.546 + t^3.454/g1^12 + g1^8*t^3.697 + g1^18*t^3.819 + g1^28*t^3.941 + t^4.362/g1^36 + t^4.483/g1^26 + (3*t^4.605)/g1^16 + (3*t^4.727)/g1^6 + 5*g1^4*t^4.849 + 2*g1^14*t^4.97 + g1^24*t^5.092 + t^5.635/g1^30 + t^5.878/g1^10 + 2*g1^10*t^6.122 + 3*g1^20*t^6.243 + 3*g1^30*t^6.365 + g1^40*t^6.487 + t^6.543/g1^54 + t^6.664/g1^44 + (3*t^6.786)/g1^34 + (4*t^6.908)/g1^24 + (5*t^7.03)/g1^14 + (5*t^7.151)/g1^4 + 6*g1^6*t^7.273 + 3*g1^16*t^7.395 + g1^26*t^7.517 + 2*g1^36*t^7.638 + g1^46*t^7.76 + t^7.816/g1^48 + g1^56*t^7.882 + t^8.059/g1^28 - (2*t^8.181)/g1^18 - 4*g1^2*t^8.424 + 2*g1^12*t^8.546 + 4*g1^22*t^8.668 + t^8.723/g1^72 + 6*g1^32*t^8.79 + t^8.845/g1^62 + 3*g1^42*t^8.911 + (3*t^8.967)/g1^52 - t^4.151/(g1^4*y) - t^6.332/(g1^22*y) - t^6.454/(g1^12*y) - (2*t^6.576)/(g1^2*y) + t^7.483/(g1^26*y) + (2*t^7.605)/(g1^16*y) + (5*t^7.727)/(g1^6*y) + (3*g1^4*t^7.849)/y + (3*g1^14*t^7.97)/y - t^8.513/(g1^40*y) - (2*t^8.757)/(g1^20*y) + t^8.878/(g1^10*y) - (t^4.151*y)/g1^4 - (t^6.332*y)/g1^22 - (t^6.454*y)/g1^12 - (2*t^6.576*y)/g1^2 + (t^7.483*y)/g1^26 + (2*t^7.605*y)/g1^16 + (5*t^7.727*y)/g1^6 + 3*g1^4*t^7.849*y + 3*g1^14*t^7.97*y - (t^8.513*y)/g1^40 - (2*t^8.757*y)/g1^20 + (t^8.878*y)/g1^10 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 2844 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{3}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ | 0.6363 | 0.7853 | 0.8103 | [X:[1.6169], M:[0.7237, 0.8085, 0.3831, 1.1492, 0.8508], q:[0.872, 0.4042], qb:[0.7449, 0.4466], phi:[0.3831]] | t^2.171 + t^2.298 + t^2.425 + t^2.553 + t^3.447 + t^3.575 + t^3.702 + t^3.829 + t^3.956 + t^4.342 + t^4.47 + 2*t^4.597 + 2*t^4.724 + 3*t^4.851 + t^4.978 + t^5.105 + t^5.619 + t^5.746 + t^5.873 + t^6. - t^4.149/y - t^4.149*y | detail |