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 |
|---|---|---|---|---|---|---|---|---|---|
| 60980 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ | 1.2074 | 1.3954 | 0.8653 | [X:[1.4573], M:[0.9071, 1.2714], q:[0.7236, 0.1809], qb:[0.5477, 0.3618], phi:[0.3643]] | [X:[[6]], M:[[-4], [-3]], q:[[-8], [-2]], qb:[[5], [-4]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{5}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ | ${}M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ 2}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 3 | t^2.19 + 2*t^2.72 + t^3.26 + t^3.28 + 3*t^3.81 + 2*t^4.35 + 2*t^4.37 + 5*t^4.91 + 5*t^5.44 + t^5.46 + 3*t^5.98 + 3*t^6. + t^6.51 + 8*t^6.54 + t^6.56 + 7*t^7.07 + 5*t^7.09 + 2*t^7.61 + 13*t^7.63 + 14*t^8.16 + 3*t^8.19 + 9*t^8.7 + 7*t^8.72 + t^8.74 - t^4.09/y - t^5.19/y - t^6.28/y - t^6.81/y - t^7.35/y - t^7.37/y - t^7.91/y + t^8.44/y - t^8.46/y + (2*t^8.98)/y - t^4.09*y - t^5.19*y - t^6.28*y - t^6.81*y - t^7.35*y - t^7.37*y - t^7.91*y + t^8.44*y - t^8.46*y + 2*t^8.98*y | g1^2*t^2.19 + t^2.72/g1^5 + t^2.72/g1^4 + t^3.26/g1^12 + g1^3*t^3.28 + t^3.81/g1^4 + (2*t^3.81)/g1^3 + (2*t^4.35)/g1^11 + g1^4*t^4.37 + g1^5*t^4.37 + (2*t^4.91)/g1^3 + (3*t^4.91)/g1^2 + (4*t^5.44)/g1^10 + t^5.44/g1^8 + g1^5*t^5.46 + (2*t^5.98)/g1^17 + t^5.98/g1^16 - 4*t^6. + (2*t^6.)/g1^2 + (5*t^6.)/g1 + t^6.51/g1^24 + (6*t^6.54)/g1^9 + t^6.54/g1^8 + t^6.54/g1^7 + 2*g1^6*t^6.56 + g1^7*t^6.56 - 2*g1^9*t^6.56 + (4*t^7.07)/g1^16 + (3*t^7.07)/g1^15 + 7*t^7.09 + (3*t^7.09)/g1 - 4*g1*t^7.09 - g1^2*t^7.09 + (2*t^7.61)/g1^23 + (8*t^7.63)/g1^8 + (3*t^7.63)/g1^7 + (2*t^7.63)/g1^6 + g1^7*t^7.65 + g1^8*t^7.65 + g1^9*t^7.65 - 3*g1^10*t^7.65 + (8*t^8.16)/g1^15 + (7*t^8.16)/g1^14 - (2*t^8.16)/g1^13 + t^8.16/g1^12 + 3*t^8.19 + 8*g1*t^8.19 - 7*g1^2*t^8.19 - g1^3*t^8.19 + g1^18*t^8.21 - g1^19*t^8.21 + (7*t^8.7)/g1^22 + t^8.7/g1^21 + t^8.7/g1^20 + (10*t^8.72)/g1^7 + (5*t^8.72)/g1^6 - (2*t^8.72)/g1^5 - (6*t^8.72)/g1^4 + 2*g1^8*t^8.74 + g1^9*t^8.74 + g1^10*t^8.74 - 5*g1^11*t^8.74 + 2*g1^12*t^8.74 - (g1*t^4.09)/y - (g1^2*t^5.19)/y - (g1^3*t^6.28)/y - t^6.81/(g1^3*y) - t^7.35/(g1^11*y) - (2*g1^4*t^7.37)/y + (g1^5*t^7.37)/y - (2*t^7.91)/(g1^2*y) + t^7.91/(g1*y) + t^8.44/(g1^9*y) - (g1^5*t^8.46)/y + t^8.98/(g1^17*y) + t^8.98/(g1^16*y) - g1*t^4.09*y - g1^2*t^5.19*y - g1^3*t^6.28*y - (t^6.81*y)/g1^3 - (t^7.35*y)/g1^11 - 2*g1^4*t^7.37*y + g1^5*t^7.37*y - (2*t^7.91*y)/g1^2 + (t^7.91*y)/g1 + (t^8.44*y)/g1^9 - g1^5*t^8.46*y + (t^8.98*y)/g1^17 + (t^8.98*y)/g1^16 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 60580 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.2273 | 1.4318 | 0.8571 | [X:[1.4545], M:[0.9091], q:[0.7273, 0.1818], qb:[0.5455, 0.3636], phi:[0.3636]] | 2*t^2.18 + 2*t^2.73 + 2*t^3.27 + 2*t^3.82 + 6*t^4.36 + 7*t^4.91 + 8*t^5.45 + 7*t^6. - t^4.09/y - t^5.18/y - t^4.09*y - t^5.18*y | detail | {a: 27/22, c: 63/44, X1: 16/11, M1: 10/11, q1: 8/11, q2: 2/11, qb1: 6/11, qb2: 4/11, phi1: 4/11} |