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 |
|---|---|---|---|---|---|---|---|---|---|
| 4530 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{7}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.623 | 0.7878 | 0.7908 | [X:[1.5907], M:[0.4093, 1.2279, 0.7721, 0.865, 1.0, 0.9536, 0.7721, 0.8186], q:[0.9093, 0.6814], qb:[0.3186, 0.4536], phi:[0.4093]] | [X:[[1]], M:[[-1], [-3], [3], [-7], [0], [5], [3], [-2]], q:[[-1], [2]], qb:[[-2], [5]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{7}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}^{2}$ | ${}$ | -2 | 2*t^2.316 + 2*t^2.456 + t^2.595 + t^2.861 + t^3. + t^3.949 + t^4.089 + 3*t^4.633 + 5*t^4.772 + 5*t^4.911 + 2*t^5.051 + 2*t^5.177 + t^5.19 + 4*t^5.316 + 2*t^5.456 + t^5.721 - 2*t^6. - t^6.139 + 2*t^6.266 + 3*t^6.405 + t^6.544 - t^6.684 + t^6.81 - t^6.823 + 5*t^6.949 + 5*t^7.089 + 8*t^7.228 + 8*t^7.367 + 2*t^7.494 + 5*t^7.506 + 6*t^7.633 + 2*t^7.646 + 6*t^7.772 + t^7.785 + t^7.898 + 2*t^7.911 + 3*t^8.038 + 2*t^8.177 - 6*t^8.316 - 8*t^8.456 + 4*t^8.582 - 5*t^8.595 + 5*t^8.721 - t^8.734 - t^4.228/y - t^6.544/y - (2*t^6.684)/y - t^6.823/y - t^7.089/y + t^7.367/y + (2*t^7.633)/y + (6*t^7.772)/y + (4*t^7.911)/y + (2*t^8.051)/y + (2*t^8.177)/y + (4*t^8.316)/y + (3*t^8.456)/y + t^8.595/y - t^4.228*y - t^6.544*y - 2*t^6.684*y - t^6.823*y - t^7.089*y + t^7.367*y + 2*t^7.633*y + 6*t^7.772*y + 4*t^7.911*y + 2*t^8.051*y + 2*t^8.177*y + 4*t^8.316*y + 3*t^8.456*y + t^8.595*y | 2*g1^3*t^2.316 + (2*t^2.456)/g1^2 + t^2.595/g1^7 + g1^5*t^2.861 + t^3. + g1^9*t^3.949 + g1^4*t^4.089 + 3*g1^6*t^4.633 + 5*g1*t^4.772 + (5*t^4.911)/g1^4 + (2*t^5.051)/g1^9 + 2*g1^8*t^5.177 + t^5.19/g1^14 + 4*g1^3*t^5.316 + (2*t^5.456)/g1^2 + g1^10*t^5.721 - 2*t^6. - t^6.139/g1^5 + 2*g1^12*t^6.266 + 3*g1^7*t^6.405 + g1^2*t^6.544 - t^6.684/g1^3 + g1^14*t^6.81 - t^6.823/g1^8 + 5*g1^9*t^6.949 + 5*g1^4*t^7.089 + (8*t^7.228)/g1 + (8*t^7.367)/g1^6 + 2*g1^11*t^7.494 + (5*t^7.506)/g1^11 + 6*g1^6*t^7.633 + (2*t^7.646)/g1^16 + 6*g1*t^7.772 + t^7.785/g1^21 + g1^18*t^7.898 + (2*t^7.911)/g1^4 + 3*g1^13*t^8.038 + 2*g1^8*t^8.177 - 6*g1^3*t^8.316 - (8*t^8.456)/g1^2 + 4*g1^15*t^8.582 - (5*t^8.595)/g1^7 + 5*g1^10*t^8.721 - t^8.734/g1^12 - t^4.228/(g1*y) - (g1^2*t^6.544)/y - (2*t^6.684)/(g1^3*y) - t^6.823/(g1^8*y) - (g1^4*t^7.089)/y + t^7.367/(g1^6*y) + (2*g1^6*t^7.633)/y + (6*g1*t^7.772)/y + (4*t^7.911)/(g1^4*y) + (2*t^8.051)/(g1^9*y) + (2*g1^8*t^8.177)/y + (4*g1^3*t^8.316)/y + (3*t^8.456)/(g1^2*y) + t^8.595/(g1^7*y) - (t^4.228*y)/g1 - g1^2*t^6.544*y - (2*t^6.684*y)/g1^3 - (t^6.823*y)/g1^8 - g1^4*t^7.089*y + (t^7.367*y)/g1^6 + 2*g1^6*t^7.633*y + 6*g1*t^7.772*y + (4*t^7.911*y)/g1^4 + (2*t^8.051*y)/g1^9 + 2*g1^8*t^8.177*y + 4*g1^3*t^8.316*y + (3*t^8.456*y)/g1^2 + (t^8.595*y)/g1^7 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2475 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{7}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ | 0.6078 | 0.7619 | 0.7977 | [X:[1.5891], M:[0.4109, 1.2328, 0.7672, 0.8766, 1.0, 0.9453, 0.7672], q:[0.9109, 0.6781], qb:[0.3219, 0.4453], phi:[0.4109]] | 2*t^2.301 + t^2.466 + t^2.63 + t^2.836 + t^3. + t^3.534 + t^3.904 + t^4.069 + 3*t^4.603 + 3*t^4.767 + 3*t^4.931 + t^5.096 + 2*t^5.137 + t^5.26 + 3*t^5.301 + t^5.466 + t^5.672 + 2*t^5.836 - t^6. - t^4.233/y - t^4.233*y | detail |