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 |
|---|---|---|---|---|---|---|---|---|---|
| 61077 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ | 1.4084 | 1.6103 | 0.8746 | [X:[1.3956], M:[0.6978, 0.6978], q:[0.6667, 0.3645], qb:[0.6355, 0.5203], phi:[0.3022]] | [X:[[2]], M:[[1], [1]], q:[[0], [1]], qb:[[-1], [6]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}q_{2}^{3}$ | -1 | 2*t^2.09 + t^2.65 + t^2.72 + t^3. + 2*t^3.56 + 4*t^4.19 + 2*t^4.47 + 2*t^4.75 + 4*t^4.81 + 2*t^5.09 + t^5.31 + 2*t^5.37 + t^5.44 + 4*t^5.65 + 2*t^5.72 + t^5.93 - t^6. + 2*t^6.22 + 9*t^6.28 - t^6.35 + 5*t^6.56 + 5*t^6.84 + 5*t^6.91 + 5*t^7.12 + 5*t^7.19 - t^7.25 + 3*t^7.4 + 6*t^7.47 + 2*t^7.53 + 8*t^7.75 + 4*t^7.81 + t^7.96 + 7*t^8.03 - 2*t^8.09 + 4*t^8.31 + 17*t^8.37 - t^8.44 + t^8.59 + 7*t^8.65 + 2*t^8.87 + 15*t^8.93 + t^8.72/y^2 - t^3.91/y - t^4.81/y - (2*t^6.)/y - t^6.56/y - t^6.63/y - (3*t^6.91)/y + t^7.19/y - (2*t^7.47)/y - t^7.53/y + (2*t^7.75)/y + (2*t^7.81)/y - t^8.09/y - t^8.37/y + (3*t^8.65)/y - t^8.72/y - t^3.91*y - t^4.81*y - 2*t^6.*y - t^6.56*y - t^6.63*y - 3*t^6.91*y + t^7.19*y - 2*t^7.47*y - t^7.53*y + 2*t^7.75*y + 2*t^7.81*y - t^8.09*y - t^8.37*y + 3*t^8.65*y - t^8.72*y + t^8.72*y^2 | 2*g1*t^2.09 + g1^7*t^2.65 + t^2.72/g1^3 + t^3. + 2*g1^6*t^3.56 + 4*g1^2*t^4.19 + 2*g1^5*t^4.47 + 2*g1^8*t^4.75 + (4*t^4.81)/g1^2 + 2*g1*t^5.09 + g1^14*t^5.31 + 2*g1^4*t^5.37 + t^5.44/g1^6 + 4*g1^7*t^5.65 + (2*t^5.72)/g1^3 + g1^10*t^5.93 - t^6. + 2*g1^13*t^6.22 + 9*g1^3*t^6.28 - t^6.35/g1^7 + 5*g1^6*t^6.56 + 5*g1^9*t^6.84 + (5*t^6.91)/g1 + 5*g1^12*t^7.12 + 5*g1^2*t^7.19 - t^7.25/g1^8 + 3*g1^15*t^7.4 + 6*g1^5*t^7.47 + (2*t^7.53)/g1^5 + 8*g1^8*t^7.75 + (4*t^7.81)/g1^2 + g1^21*t^7.96 + 7*g1^11*t^8.03 - 2*g1*t^8.09 + 4*g1^14*t^8.31 + 17*g1^4*t^8.37 - t^8.44/g1^6 + g1^17*t^8.59 + 7*g1^7*t^8.65 + 2*g1^20*t^8.87 + 15*g1^10*t^8.93 + t^8.72/(g1^3*y^2) - t^3.91/(g1*y) - t^4.81/(g1^2*y) - (2*t^6.)/y - (g1^6*t^6.56)/y - t^6.63/(g1^4*y) - (3*t^6.91)/(g1*y) + (g1^2*t^7.19)/y - (2*g1^5*t^7.47)/y - t^7.53/(g1^5*y) + (2*g1^8*t^7.75)/y + (2*t^7.81)/(g1^2*y) - (g1*t^8.09)/y - (g1^4*t^8.37)/y + (3*g1^7*t^8.65)/y - t^8.72/(g1^3*y) - (t^3.91*y)/g1 - (t^4.81*y)/g1^2 - 2*t^6.*y - g1^6*t^6.56*y - (t^6.63*y)/g1^4 - (3*t^6.91*y)/g1 + g1^2*t^7.19*y - 2*g1^5*t^7.47*y - (t^7.53*y)/g1^5 + 2*g1^8*t^7.75*y + (2*t^7.81*y)/g1^2 - g1*t^8.09*y - g1^4*t^8.37*y + 3*g1^7*t^8.65*y - (t^8.72*y)/g1^3 + (t^8.72*y^2)/g1^3 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 60132 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ | 1.4182 | 1.6227 | 0.874 | [X:[1.3635], M:[0.774, 0.774], q:[0.6667, 0.3484], qb:[0.5593, 0.516], phi:[0.3183]] | 2*t^2.32 + t^2.59 + t^2.72 + t^2.86 + 2*t^3.55 + t^4.09 + 2*t^4.5 + 2*t^4.63 + 3*t^4.64 + 2*t^4.92 + 2*t^5.05 + 3*t^5.19 + t^5.32 + t^5.45 + 2*t^5.46 + 2*t^5.59 + 2*t^5.73 + t^5.86 + 3*t^5.87 - 2*t^6. - t^3.95/y - t^4.91/y - t^3.95*y - t^4.91*y | detail |