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 |
|---|---|---|---|---|---|---|---|---|---|
| 56883 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}X_{1}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ | 0.6036 | 0.7534 | 0.8013 | [X:[1.4069], M:[1.1863, 0.9886, 0.8137, 0.5931, 1.0114, 0.8137, 0.768], q:[0.2966, 0.5171], qb:[0.7149, 0.8897], phi:[0.3954]] | [X:[[6]], M:[[-12], [-10], [12], [-6], [10], [12], [-28]], q:[[-3], [15]], qb:[[13], [-9]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{7}\phi_{1}q_{1}q_{2}$ | ${}\phi_{1}^{3}q_{1}q_{2}$ | -1 | t^2.304 + t^2.373 + 2*t^2.441 + t^2.966 + t^3.034 + t^3.627 + t^4.221 + t^4.289 + t^4.608 + t^4.677 + 3*t^4.745 + 3*t^4.814 + 3*t^4.882 + t^5.27 + t^5.338 + 2*t^5.407 + 2*t^5.475 + t^5.931 - t^6. + 2*t^6.069 + 2*t^6.662 + 2*t^6.73 + t^6.912 + t^6.981 + 3*t^7.049 + 3*t^7.118 + 4*t^7.186 + 4*t^7.255 + 4*t^7.323 + t^7.574 + t^7.642 + 2*t^7.711 + t^7.779 + 2*t^7.848 + 3*t^7.917 + t^8.235 - 2*t^8.304 - t^8.373 - 3*t^8.441 + 3*t^8.51 + t^8.578 - 2*t^8.966 - t^4.186/y - t^6.49/y - t^6.559/y - t^6.627/y + t^7.677/y + (3*t^7.745)/y + (3*t^7.814)/y + (2*t^7.882)/y + t^8.27/y + (2*t^8.338)/y + (3*t^8.407)/y + (2*t^8.475)/y - t^8.794/y - t^8.863/y - t^8.931/y - t^4.186*y - t^6.49*y - t^6.559*y - t^6.627*y + t^7.677*y + 3*t^7.745*y + 3*t^7.814*y + 2*t^7.882*y + t^8.27*y + 2*t^8.338*y + 3*t^8.407*y + 2*t^8.475*y - t^8.794*y - t^8.863*y - t^8.931*y | t^2.304/g1^28 + t^2.373/g1^8 + 2*g1^12*t^2.441 + t^2.966/g1^10 + g1^10*t^3.034 + g1^8*t^3.627 + g1^6*t^4.221 + g1^26*t^4.289 + t^4.608/g1^56 + t^4.677/g1^36 + (3*t^4.745)/g1^16 + 3*g1^4*t^4.814 + 3*g1^24*t^4.882 + t^5.27/g1^38 + t^5.338/g1^18 + 2*g1^2*t^5.407 + 2*g1^22*t^5.475 + t^5.931/g1^20 - t^6. + 2*g1^20*t^6.069 + 2*g1^18*t^6.662 + 2*g1^38*t^6.73 + t^6.912/g1^84 + t^6.981/g1^64 + (3*t^7.049)/g1^44 + (3*t^7.118)/g1^24 + (4*t^7.186)/g1^4 + 4*g1^16*t^7.255 + 4*g1^36*t^7.323 + t^7.574/g1^66 + t^7.642/g1^46 + (2*t^7.711)/g1^26 + t^7.779/g1^6 + 2*g1^14*t^7.848 + 3*g1^34*t^7.917 + t^8.235/g1^48 - (2*t^8.304)/g1^28 - t^8.373/g1^8 - 3*g1^12*t^8.441 + 3*g1^32*t^8.51 + g1^52*t^8.578 - (2*t^8.966)/g1^10 - t^4.186/(g1^4*y) - t^6.49/(g1^32*y) - t^6.559/(g1^12*y) - (g1^8*t^6.627)/y + t^7.677/(g1^36*y) + (3*t^7.745)/(g1^16*y) + (3*g1^4*t^7.814)/y + (2*g1^24*t^7.882)/y + t^8.27/(g1^38*y) + (2*t^8.338)/(g1^18*y) + (3*g1^2*t^8.407)/y + (2*g1^22*t^8.475)/y - t^8.794/(g1^60*y) - t^8.863/(g1^40*y) - t^8.931/(g1^20*y) - (t^4.186*y)/g1^4 - (t^6.49*y)/g1^32 - (t^6.559*y)/g1^12 - g1^8*t^6.627*y + (t^7.677*y)/g1^36 + (3*t^7.745*y)/g1^16 + 3*g1^4*t^7.814*y + 2*g1^24*t^7.882*y + (t^8.27*y)/g1^38 + (2*t^8.338*y)/g1^18 + 3*g1^2*t^8.407*y + 2*g1^22*t^8.475*y - (t^8.794*y)/g1^60 - (t^8.863*y)/g1^40 - (t^8.931*y)/g1^20 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55236 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}X_{1}$ + ${ }M_{1}M_{6}$ | 0.5867 | 0.7259 | 0.8083 | [X:[1.3951], M:[1.2097, 1.0081, 0.7903, 0.6049, 0.9919, 0.7903], q:[0.3024, 0.4879], qb:[0.6895, 0.9073], phi:[0.4032]] | 2*t^2.371 + t^2.419 + t^2.976 + t^3.024 + t^3.532 + t^3.581 + t^4.137 + t^4.185 + 3*t^4.742 + 3*t^4.79 + t^4.839 + 2*t^5.347 + 2*t^5.395 + 2*t^5.903 + 3*t^5.951 - t^6. - t^4.21/y - t^4.21*y | detail |