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 |
|---|---|---|---|---|---|---|---|---|---|
| 56727 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6642 | 0.8311 | 0.7992 | [M:[1.1648, 1.0879, 0.8352, 0.8022, 1.0549, 0.6923, 1.0549], q:[0.4011, 0.4341], qb:[0.511, 0.7637], phi:[0.4725]] | [M:[[12], [-30], [-12], [22], [4], [14], [4]], q:[[11], [-23]], qb:[[19], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{4}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.077 + t^2.407 + t^2.506 + 2*t^3.165 + t^3.264 + t^3.494 + 2*t^3.824 + t^4.022 + 2*t^4.154 + t^4.253 + 2*t^4.483 + t^4.582 + t^4.813 + t^4.912 + t^5.011 + 2*t^5.242 + t^5.341 + 3*t^5.571 + 2*t^5.67 + 2*t^5.901 - 2*t^6. + 3*t^6.231 + 3*t^6.33 + 2*t^6.429 + 2*t^6.528 + 3*t^6.56 + 3*t^6.659 + 2*t^6.89 + 4*t^6.989 + t^7.22 + t^7.286 + 5*t^7.319 + t^7.418 + t^7.517 + 6*t^7.648 + t^7.747 + 6*t^7.978 + t^8.044 - t^8.077 + t^8.275 + 5*t^8.308 - t^8.407 + t^8.604 + 5*t^8.637 + 5*t^8.736 + 2*t^8.835 + t^8.934 + 4*t^8.967 - t^4.418/y - t^6.494/y - t^6.824/y + t^7.154/y + t^7.253/y + t^7.483/y - t^7.681/y + t^7.912/y + t^8.011/y + (2*t^8.242)/y + (2*t^8.341)/y + (2*t^8.571)/y + (3*t^8.67)/y + t^8.769/y + (2*t^8.901)/y - t^4.418*y - t^6.494*y - t^6.824*y + t^7.154*y + t^7.253*y + t^7.483*y - t^7.681*y + t^7.912*y + t^8.011*y + 2*t^8.242*y + 2*t^8.341*y + 2*t^8.571*y + 3*t^8.67*y + t^8.769*y + 2*t^8.901*y | g1^14*t^2.077 + g1^22*t^2.407 + t^2.506/g1^12 + 2*g1^4*t^3.165 + t^3.264/g1^30 + g1^12*t^3.494 + 2*g1^20*t^3.824 + t^4.022/g1^48 + 2*g1^28*t^4.154 + t^4.253/g1^6 + 2*g1^36*t^4.483 + g1^2*t^4.582 + g1^44*t^4.813 + g1^10*t^4.912 + t^5.011/g1^24 + 2*g1^18*t^5.242 + t^5.341/g1^16 + 3*g1^26*t^5.571 + (2*t^5.67)/g1^8 + 2*g1^34*t^5.901 - 2*t^6. + 3*g1^42*t^6.231 + 3*g1^8*t^6.33 + (2*t^6.429)/g1^26 + (2*t^6.528)/g1^60 + 3*g1^50*t^6.56 + 3*g1^16*t^6.659 + 2*g1^58*t^6.89 + 4*g1^24*t^6.989 + g1^66*t^7.22 + t^7.286/g1^78 + 5*g1^32*t^7.319 + t^7.418/g1^2 + t^7.517/g1^36 + 6*g1^40*t^7.648 + g1^6*t^7.747 + 6*g1^48*t^7.978 + t^8.044/g1^96 - g1^14*t^8.077 + t^8.275/g1^54 + 5*g1^56*t^8.308 - g1^22*t^8.407 + t^8.604/g1^46 + 5*g1^64*t^8.637 + 5*g1^30*t^8.736 + (2*t^8.835)/g1^4 + t^8.934/g1^38 + 4*g1^72*t^8.967 - t^4.418/(g1^2*y) - (g1^12*t^6.494)/y - (g1^20*t^6.824)/y + (g1^28*t^7.154)/y + t^7.253/(g1^6*y) + (g1^36*t^7.483)/y - t^7.681/(g1^32*y) + (g1^10*t^7.912)/y + t^8.011/(g1^24*y) + (2*g1^18*t^8.242)/y + (2*t^8.341)/(g1^16*y) + (2*g1^26*t^8.571)/y + (3*t^8.67)/(g1^8*y) + t^8.769/(g1^42*y) + (2*g1^34*t^8.901)/y - (t^4.418*y)/g1^2 - g1^12*t^6.494*y - g1^20*t^6.824*y + g1^28*t^7.154*y + (t^7.253*y)/g1^6 + g1^36*t^7.483*y - (t^7.681*y)/g1^32 + g1^10*t^7.912*y + (t^8.011*y)/g1^24 + 2*g1^18*t^8.242*y + (2*t^8.341*y)/g1^16 + 2*g1^26*t^8.571*y + (3*t^8.67*y)/g1^8 + (t^8.769*y)/g1^42 + 2*g1^34*t^8.901*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55099 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}^{2}$ | 0.6693 | 0.8394 | 0.7974 | [M:[1.167, 1.0824, 0.833, 0.8062, 1.0557, 0.6949], q:[0.4031, 0.4299], qb:[0.5145, 0.7639], phi:[0.4722]] | t^2.085 + t^2.419 + t^2.499 + t^2.833 + t^3.167 + t^3.247 + t^3.501 + 2*t^3.835 + t^3.996 + 2*t^4.169 + t^4.249 + 2*t^4.503 + t^4.584 + t^4.837 + 2*t^4.918 + t^4.998 + 2*t^5.252 + 2*t^5.332 + 2*t^5.586 + 2*t^5.666 + 2*t^5.92 - t^6. - t^4.416/y - t^4.416*y | detail |