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 |
|---|---|---|---|---|---|---|---|---|---|
| 58108 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.44 | 1.6325 | 0.8821 | [X:[1.3245], M:[0.9734], q:[0.4282, 0.4548], qb:[0.5718, 0.5186], phi:[0.3378]] | [X:[[6]], M:[[18]], q:[[11], [-7]], qb:[[-11], [25]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}$ | -2 | t^2.84 + 2*t^2.92 + t^3. + t^3.04 + t^3.85 + t^3.93 + t^3.97 + t^4.01 + t^4.09 + t^4.87 + 2*t^4.95 + 2*t^5.03 + t^5.11 + t^5.68 + 2*t^5.76 + 4*t^5.84 + t^5.88 + t^5.92 + 3*t^5.96 - 2*t^6. + 2*t^6.04 - t^6.16 + t^6.69 + 3*t^6.77 + t^6.81 + 4*t^6.85 + 4*t^6.89 + 2*t^6.93 + 3*t^6.97 + 2*t^7.01 + 2*t^7.05 - t^7.09 + 2*t^7.13 - t^7.17 + 3*t^7.71 + 5*t^7.79 + 8*t^7.87 + 6*t^7.95 + t^7.99 + 3*t^8.03 + 2*t^8.07 - t^8.11 + t^8.15 + t^8.52 + 2*t^8.6 + 4*t^8.68 + 2*t^8.72 + 4*t^8.76 + 6*t^8.8 - 2*t^8.84 + 10*t^8.88 - 6*t^8.92 + 7*t^8.96 - t^4.01/y - t^5.03/y - t^6.85/y - (2*t^6.93)/y - t^7.01/y - t^7.05/y - t^7.87/y - (2*t^7.95)/y - t^8.03/y - t^8.07/y + (2*t^8.76)/y + (2*t^8.84)/y + (2*t^8.92)/y + t^8.96/y - t^4.01*y - t^5.03*y - t^6.85*y - 2*t^6.93*y - t^7.01*y - t^7.05*y - t^7.87*y - 2*t^7.95*y - t^8.03*y - t^8.07*y + 2*t^8.76*y + 2*t^8.84*y + 2*t^8.92*y + t^8.96*y | g1^36*t^2.84 + 2*g1^18*t^2.92 + t^3. + t^3.04/g1^9 + g1^33*t^3.85 + g1^15*t^3.93 + g1^6*t^3.97 + t^4.01/g1^3 + t^4.09/g1^21 + g1^30*t^4.87 + 2*g1^12*t^4.95 + (2*t^5.03)/g1^6 + t^5.11/g1^24 + g1^72*t^5.68 + 2*g1^54*t^5.76 + 4*g1^36*t^5.84 + g1^27*t^5.88 + g1^18*t^5.92 + 3*g1^9*t^5.96 - 2*t^6. + (2*t^6.04)/g1^9 - t^6.16/g1^36 + g1^69*t^6.69 + 3*g1^51*t^6.77 + g1^42*t^6.81 + 4*g1^33*t^6.85 + 4*g1^24*t^6.89 + 2*g1^15*t^6.93 + 3*g1^6*t^6.97 + (2*t^7.01)/g1^3 + (2*t^7.05)/g1^12 - t^7.09/g1^21 + (2*t^7.13)/g1^30 - t^7.17/g1^39 + 3*g1^66*t^7.71 + 5*g1^48*t^7.79 + 8*g1^30*t^7.87 + 6*g1^12*t^7.95 + g1^3*t^7.99 + (3*t^8.03)/g1^6 + (2*t^8.07)/g1^15 - t^8.11/g1^24 + t^8.15/g1^33 + g1^108*t^8.52 + 2*g1^90*t^8.6 + 4*g1^72*t^8.68 + 2*g1^63*t^8.72 + 4*g1^54*t^8.76 + 6*g1^45*t^8.8 - 2*g1^36*t^8.84 + 10*g1^27*t^8.88 - 6*g1^18*t^8.92 + 7*g1^9*t^8.96 - t^4.01/(g1^3*y) - t^5.03/(g1^6*y) - (g1^33*t^6.85)/y - (2*g1^15*t^6.93)/y - t^7.01/(g1^3*y) - t^7.05/(g1^12*y) - (g1^30*t^7.87)/y - (2*g1^12*t^7.95)/y - t^8.03/(g1^6*y) - t^8.07/(g1^15*y) + (2*g1^54*t^8.76)/y + (2*g1^36*t^8.84)/y + (2*g1^18*t^8.92)/y + (g1^9*t^8.96)/y - (t^4.01*y)/g1^3 - (t^5.03*y)/g1^6 - g1^33*t^6.85*y - 2*g1^15*t^6.93*y - (t^7.01*y)/g1^3 - (t^7.05*y)/g1^12 - g1^30*t^7.87*y - 2*g1^12*t^7.95*y - (t^8.03*y)/g1^6 - (t^8.07*y)/g1^15 + 2*g1^54*t^8.76*y + 2*g1^36*t^8.84*y + 2*g1^18*t^8.92*y + g1^9*t^8.96*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57335 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4541 | 1.6446 | 0.8841 | [X:[1.3279], M:[0.9838], q:[0.4878, 0.5039], qb:[0.5122, 0.4799], phi:[0.336]] | t^2.903 + 2*t^2.951 + t^3. + t^3.024 + t^3.911 + t^3.96 + t^3.984 + t^4.008 + t^4.057 + t^4.919 + t^4.968 + t^5.016 + t^5.065 + t^5.424 + t^5.447 + t^5.495 + t^5.521 + t^5.806 + 2*t^5.854 + 3*t^5.903 + t^5.927 + t^5.951 + 2*t^5.976 - 3*t^6. - t^4.008/y - t^5.016/y - t^4.008*y - t^5.016*y | detail |