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 |
|---|---|---|---|---|---|---|---|---|---|
| 57059 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{2}M_{5}$ + ${ }M_{2}M_{7}$ | 0.5828 | 0.7356 | 0.7924 | [X:[1.5704], M:[0.4296, 1.007, 1.2887, 0.7113, 0.993, 0.7113, 0.993], q:[0.6444, 0.9261], qb:[0.3486, 0.3627], phi:[0.4296]] | [X:[[2]], M:[[-2], [-14], [-6], [6], [14], [6], [14]], q:[[-3], [5]], qb:[[17], [-11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$ | ${}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | 2*t^2.134 + t^2.577 + 2*t^2.979 + t^3.38 + t^3.423 + t^3.465 + t^3.824 + 3*t^4.268 + 3*t^4.711 + 4*t^5.113 + t^5.155 + 2*t^5.514 + 3*t^5.556 + t^5.598 + 5*t^5.958 - 2*t^6. + 2*t^6.359 + 5*t^6.402 + t^6.761 + 2*t^6.803 + 3*t^6.845 - t^6.887 + t^6.929 + t^7.205 + 5*t^7.247 + t^7.289 - t^7.331 + 4*t^7.648 + 5*t^7.69 + 9*t^8.092 - 4*t^8.134 - t^8.176 + 4*t^8.493 + 8*t^8.535 - 4*t^8.577 + 2*t^8.895 + 7*t^8.937 - 2*t^8.979 - t^4.289/y - t^6.423/y - t^6.866/y + t^7.31/y + (3*t^7.711)/y + (4*t^8.113)/y + t^8.155/y + (2*t^8.514)/y + (3*t^8.556)/y + (2*t^8.598)/y + (4*t^8.958)/y - t^4.289*y - t^6.423*y - t^6.866*y + t^7.31*y + 3*t^7.711*y + 4*t^8.113*y + t^8.155*y + 2*t^8.514*y + 3*t^8.556*y + 2*t^8.598*y + 4*t^8.958*y | 2*g1^6*t^2.134 + t^2.577/g1^4 + 2*g1^14*t^2.979 + g1^32*t^3.38 + g1^4*t^3.423 + t^3.465/g1^24 + g1^22*t^3.824 + 3*g1^12*t^4.268 + 3*g1^2*t^4.711 + 4*g1^20*t^5.113 + t^5.155/g1^8 + 2*g1^38*t^5.514 + 3*g1^10*t^5.556 + t^5.598/g1^18 + 5*g1^28*t^5.958 - 2*t^6. + 2*g1^46*t^6.359 + 5*g1^18*t^6.402 + g1^64*t^6.761 + 2*g1^36*t^6.803 + 3*g1^8*t^6.845 - t^6.887/g1^20 + t^6.929/g1^48 + g1^54*t^7.205 + 5*g1^26*t^7.247 + t^7.289/g1^2 - t^7.331/g1^30 + 4*g1^44*t^7.648 + 5*g1^16*t^7.69 + 9*g1^34*t^8.092 - 4*g1^6*t^8.134 - t^8.176/g1^22 + 4*g1^52*t^8.493 + 8*g1^24*t^8.535 - (4*t^8.577)/g1^4 + 2*g1^70*t^8.895 + 7*g1^42*t^8.937 - 2*g1^14*t^8.979 - t^4.289/(g1^2*y) - (g1^4*t^6.423)/y - t^6.866/(g1^6*y) + t^7.31/(g1^16*y) + (3*g1^2*t^7.711)/y + (4*g1^20*t^8.113)/y + t^8.155/(g1^8*y) + (2*g1^38*t^8.514)/y + (3*g1^10*t^8.556)/y + (2*t^8.598)/(g1^18*y) + (4*g1^28*t^8.958)/y - (t^4.289*y)/g1^2 - g1^4*t^6.423*y - (t^6.866*y)/g1^6 + (t^7.31*y)/g1^16 + 3*g1^2*t^7.711*y + 4*g1^20*t^8.113*y + (t^8.155*y)/g1^8 + 2*g1^38*t^8.514*y + 3*g1^10*t^8.556*y + (2*t^8.598*y)/g1^18 + 4*g1^28*t^8.958*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55459 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{2}M_{5}$ | 0.5831 | 0.734 | 0.7944 | [X:[1.5732], M:[0.4268, 0.9873, 1.2803, 0.7197, 1.0127, 0.7197], q:[0.6401, 0.9331], qb:[0.3725, 0.3472], phi:[0.4268]] | 2*t^2.159 + t^2.561 + t^2.962 + t^3.038 + t^3.363 + t^3.439 + t^3.516 + t^3.917 + 3*t^4.318 + 3*t^4.72 + 3*t^5.121 + 2*t^5.197 + 2*t^5.523 + 2*t^5.599 + 2*t^5.675 + t^5.924 - t^6. - t^4.28/y - t^4.28*y | detail |