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 |
|---|---|---|---|---|---|---|---|---|---|
| 59450 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.3616 | 1.5707 | 0.8668 | [X:[1.2871], M:[0.9307], q:[0.5511, 0.264], qb:[0.4489, 0.5973], phi:[0.3564]] | [X:[[2]], M:[[3]], q:[[5], [3]], qb:[[-5], [3]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}q_{2}\tilde{q}_{1}X_{1}$ | 0 | t^2.14 + t^2.58 + t^2.79 + t^3. + t^3.21 + t^3.45 + t^3.65 + t^3.86 + t^4.07 + 2*t^4.28 + t^4.31 + t^4.51 + 2*t^4.72 + t^4.93 + t^5.14 + 2*t^5.17 + t^5.35 + 2*t^5.38 + 5*t^5.58 + 3*t^5.79 + t^6.03 + t^6.21 + 3*t^6.24 + 3*t^6.42 + 4*t^6.45 + 4*t^6.65 + 4*t^6.86 + 2*t^6.89 + t^7.07 + 2*t^7.1 + t^7.25 + 2*t^7.28 + 7*t^7.31 + t^7.49 + 5*t^7.51 + 7*t^7.72 + 3*t^7.75 + 3*t^7.93 + 5*t^7.96 - t^8.11 + 8*t^8.17 + t^8.35 + 9*t^8.38 + 3*t^8.55 + 7*t^8.58 + 3*t^8.61 + 4*t^8.79 + 5*t^8.82 - t^8.97 - t^4.07/y - t^5.14/y - t^6.21/y - t^6.65/y - t^6.86/y - t^7.07/y - t^7.28/y - t^7.51/y - t^8.35/y + t^8.38/y + t^8.58/y + t^8.79/y - t^4.07*y - t^5.14*y - t^6.21*y - t^6.65*y - t^6.86*y - t^7.07*y - t^7.28*y - t^7.51*y - t^8.35*y + t^8.38*y + t^8.58*y + t^8.79*y | t^2.14/g1^2 + g1^6*t^2.58 + g1^3*t^2.79 + t^3. + t^3.21/g1^3 + g1^8*t^3.45 + g1^5*t^3.65 + g1^2*t^3.86 + t^4.07/g1 + (2*t^4.28)/g1^4 + g1^10*t^4.31 + g1^7*t^4.51 + 2*g1^4*t^4.72 + g1*t^4.93 + t^5.14/g1^2 + 2*g1^12*t^5.17 + t^5.35/g1^5 + 2*g1^9*t^5.38 + 5*g1^6*t^5.58 + 3*g1^3*t^5.79 + g1^14*t^6.03 + t^6.21/g1^3 + 3*g1^11*t^6.24 + (3*t^6.42)/g1^6 + 4*g1^8*t^6.45 + 4*g1^5*t^6.65 + 4*g1^2*t^6.86 + 2*g1^16*t^6.89 + t^7.07/g1 + 2*g1^13*t^7.1 + t^7.25/g1^18 + (2*t^7.28)/g1^4 + 7*g1^10*t^7.31 + t^7.49/g1^7 + 5*g1^7*t^7.51 + 7*g1^4*t^7.72 + 3*g1^18*t^7.75 + 3*g1*t^7.93 + 5*g1^15*t^7.96 - t^8.11/g1^16 + 8*g1^12*t^8.17 + t^8.35/g1^5 + 9*g1^9*t^8.38 + (3*t^8.55)/g1^8 + 7*g1^6*t^8.58 + 3*g1^20*t^8.61 + 4*g1^3*t^8.79 + 5*g1^17*t^8.82 - t^8.97/g1^14 - t^4.07/(g1*y) - t^5.14/(g1^2*y) - t^6.21/(g1^3*y) - (g1^5*t^6.65)/y - (g1^2*t^6.86)/y - t^7.07/(g1*y) - t^7.28/(g1^4*y) - (g1^7*t^7.51)/y - t^8.35/(g1^5*y) + (g1^9*t^8.38)/y + (g1^6*t^8.58)/y + (g1^3*t^8.79)/y - (t^4.07*y)/g1 - (t^5.14*y)/g1^2 - (t^6.21*y)/g1^3 - g1^5*t^6.65*y - g1^2*t^6.86*y - (t^7.07*y)/g1 - (t^7.28*y)/g1^4 - g1^7*t^7.51*y - (t^8.35*y)/g1^5 + g1^9*t^8.38*y + g1^6*t^8.58*y + g1^3*t^8.79*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57417 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4634 | 1.6643 | 0.8793 | [X:[1.3522], M:[0.6722], q:[0.4764, 0.4803], qb:[0.5236, 0.5763], phi:[0.3239]] | t^2.017 + t^2.915 + t^3. + t^3.012 + t^3.158 + t^3.17 + t^3.972 + t^4.033 + t^4.057 + t^4.13 + t^4.141 + t^4.932 + t^4.943 + t^4.955 + t^5.017 + t^5.028 + t^5.102 + t^5.113 + t^5.175 + t^5.186 + t^5.271 + t^5.283 + t^5.83 + t^5.915 + t^5.927 - 2*t^6. - t^3.972/y - t^4.943/y - t^5.988/y - t^3.972*y - t^4.943*y - t^5.988*y | detail |