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 |
|---|---|---|---|---|---|---|---|---|---|
| 58964 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.1327 | 1.3367 | 0.8474 | [X:[1.595], M:[1.1901], q:[0.1515, 0.4821], qb:[0.6832, 0.2534], phi:[0.405]] | [X:[[3]], M:[[6]], q:[[-11], [31]], qb:[[-10], [8]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ | ${2}\phi_{1}^{3}q_{1}^{2}q_{2}$ | 0 | t^2.21 + t^2.43 + t^2.5 + t^3.42 + t^3.5 + 2*t^3.57 + 2*t^3.64 + t^3.72 + t^4.41 + t^4.56 + 2*t^4.64 + t^4.71 + 3*t^4.79 + t^4.86 + 2*t^4.93 + t^5.01 + t^5.63 + t^5.7 + 3*t^5.78 + 2*t^5.85 + 4*t^5.93 + 4*t^6.07 + 3*t^6.15 + t^6.62 + t^6.77 + 3*t^6.84 + 2*t^6.92 + 5*t^6.99 + 5*t^7.07 + 5*t^7.14 + 5*t^7.21 + 6*t^7.29 + t^7.36 + 2*t^7.44 + t^7.51 + t^7.83 + t^7.91 + 5*t^7.98 + 3*t^8.06 + 6*t^8.13 + 4*t^8.21 + 6*t^8.28 + 6*t^8.36 + 4*t^8.43 + 3*t^8.5 + 3*t^8.58 + 3*t^8.65 + t^8.83 + t^8.98 - t^4.21/y - t^5.43/y - t^6.42/y - t^6.72/y - (2*t^7.86)/y + t^8.7/y + (2*t^8.78)/y + (2*t^8.85)/y + (3*t^8.93)/y - t^4.21*y - t^5.43*y - t^6.42*y - t^6.72*y - 2*t^7.86*y + t^8.7*y + 2*t^8.78*y + 2*t^8.85*y + 3*t^8.93*y | g1^39*t^2.21 + t^2.43/g1^6 + t^2.5/g1^21 + g1^36*t^3.42 + g1^21*t^3.5 + 2*g1^6*t^3.57 + (2*t^3.64)/g1^9 + t^3.72/g1^24 + g1^78*t^4.41 + g1^48*t^4.56 + 2*g1^33*t^4.64 + g1^18*t^4.71 + 3*g1^3*t^4.79 + t^4.86/g1^12 + (2*t^4.93)/g1^27 + t^5.01/g1^42 + g1^75*t^5.63 + g1^60*t^5.7 + 3*g1^45*t^5.78 + 2*g1^30*t^5.85 + 4*g1^15*t^5.93 + (4*t^6.07)/g1^15 + (3*t^6.15)/g1^30 + g1^117*t^6.62 + g1^87*t^6.77 + 3*g1^72*t^6.84 + 2*g1^57*t^6.92 + 5*g1^42*t^6.99 + 5*g1^27*t^7.07 + 5*g1^12*t^7.14 + (5*t^7.21)/g1^3 + (6*t^7.29)/g1^18 + t^7.36/g1^33 + (2*t^7.44)/g1^48 + t^7.51/g1^63 + g1^114*t^7.83 + g1^99*t^7.91 + 5*g1^84*t^7.98 + 3*g1^69*t^8.06 + 6*g1^54*t^8.13 + 4*g1^39*t^8.21 + 6*g1^24*t^8.28 + 6*g1^9*t^8.36 + (4*t^8.43)/g1^6 + (3*t^8.5)/g1^21 + (3*t^8.58)/g1^36 + (3*t^8.65)/g1^51 + g1^156*t^8.83 + g1^126*t^8.98 - t^4.21/(g1^3*y) - t^5.43/(g1^6*y) - (g1^36*t^6.42)/y - t^6.72/(g1^24*y) - (2*t^7.86)/(g1^12*y) + (g1^60*t^8.7)/y + (2*g1^45*t^8.78)/y + (2*g1^30*t^8.85)/y + (3*g1^15*t^8.93)/y - (t^4.21*y)/g1^3 - (t^5.43*y)/g1^6 - g1^36*t^6.42*y - (t^6.72*y)/g1^24 - (2*t^7.86*y)/g1^12 + g1^60*t^8.7*y + 2*g1^45*t^8.78*y + 2*g1^30*t^8.85*y + 3*g1^15*t^8.93*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57728 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ | 1.1613 | 1.3662 | 0.85 | [X:[1.594], M:[1.1879], q:[0.2239, 0.5394], qb:[0.6183, 0.1822], phi:[0.406]] | t^2.16 + t^2.44 + t^2.53 + t^3.38 + t^3.47 + t^3.56 + 2*t^3.65 + t^3.74 + t^4.17 + t^4.18 + t^4.33 + 2*t^4.6 + t^4.69 + t^4.78 + t^4.87 + 2*t^4.96 + t^5.13 + t^5.29 + t^5.38 + t^5.4 + t^5.47 + t^5.55 + t^5.64 + t^5.67 + t^5.73 + 3*t^5.82 + 3*t^5.91 - 3*t^6. - t^4.22/y - t^5.44/y - t^4.22*y - t^5.44*y | detail |