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 |
|---|---|---|---|---|---|---|---|---|---|
| 166 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6571 | 0.8446 | 0.778 | [M:[1.1432, 0.6784, 0.6784], q:[0.75, 0.4284], qb:[0.4284, 0.3932], phi:[0.5]] | [M:[[0, 1], [1, 0], [-1, -1]], q:[[0, 0], [-1, -1]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}q_{1}q_{2}^{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | -1 | 2*t^2.035 + 2*t^2.465 + t^3. + 2*t^3.43 + 2*t^3.535 + t^3.859 + 6*t^4.07 + 4*t^4.5 + 3*t^4.93 + 2*t^5.035 + 6*t^5.465 + 4*t^5.57 + 4*t^5.894 - t^6. + 8*t^6.106 + 2*t^6.324 + 10*t^6.535 + 3*t^6.859 + 6*t^6.965 + 5*t^7.07 + 2*t^7.289 + 2*t^7.394 + 8*t^7.5 + 8*t^7.606 + t^7.719 + 9*t^7.93 - 6*t^8.035 + 15*t^8.141 + 6*t^8.359 - 4*t^8.465 + 12*t^8.57 + 3*t^8.789 + 4*t^8.894 - t^4.5/y - (2*t^6.535)/y + (2*t^7.07)/y + (4*t^7.5)/y + (2*t^8.035)/y + (8*t^8.465)/y + t^8.57/y + (6*t^8.894)/y - t^4.5*y - 2*t^6.535*y + 2*t^7.07*y + 4*t^7.5*y + 2*t^8.035*y + 8*t^8.465*y + t^8.57*y + 6*t^8.894*y | g1*t^2.035 + t^2.035/(g1*g2) + t^2.465/g1 + g1*g2*t^2.465 + t^3. + 2*g2*t^3.43 + g1*t^3.535 + t^3.535/(g1*g2) + g2^2*t^3.859 + 2*g1^2*t^4.07 + (2*t^4.07)/(g1^2*g2^2) + (2*t^4.07)/g2 + 2*t^4.5 + t^4.5/(g1^2*g2) + g1^2*g2*t^4.5 + t^4.93/g1^2 + g2*t^4.93 + g1^2*g2^2*t^4.93 + g1*t^5.035 + t^5.035/(g1*g2) + (3*t^5.465)/g1 + 3*g1*g2*t^5.465 + g1^2*t^5.57 + t^5.57/(g1^2*g2^2) + (2*t^5.57)/g2 + (2*g2*t^5.894)/g1 + 2*g1*g2^2*t^5.894 - t^6. + 2*g1^3*t^6.106 + (2*t^6.106)/(g1^3*g2^3) + (2*t^6.106)/(g1*g2^2) + (2*g1*t^6.106)/g2 + (g2^2*t^6.324)/g1 + g1*g2^3*t^6.324 + 3*g1*t^6.535 + (2*t^6.535)/(g1^3*g2^2) + (3*t^6.535)/(g1*g2) + 2*g1^3*g2*t^6.535 + 3*g2^2*t^6.859 + (2*t^6.965)/g1 + t^6.965/(g1^3*g2) + 2*g1*g2*t^6.965 + g1^3*g2^2*t^6.965 + 2*g1^2*t^7.07 + (2*t^7.07)/(g1^2*g2^2) + t^7.07/g2 + 2*g2^3*t^7.289 + t^7.394/g1^3 + g1^3*g2^3*t^7.394 + 2*t^7.5 + (3*t^7.5)/(g1^2*g2) + 3*g1^2*g2*t^7.5 + 2*g1^3*t^7.606 + (2*t^7.606)/(g1^3*g2^3) + (2*t^7.606)/(g1*g2^2) + (2*g1*t^7.606)/g2 + g2^4*t^7.719 + (3*t^7.93)/g1^2 + 3*g2*t^7.93 + 3*g1^2*g2^2*t^7.93 - 3*g1*t^8.035 - (3*t^8.035)/(g1*g2) + 3*g1^4*t^8.141 + (3*t^8.141)/(g1^4*g2^4) + (3*t^8.141)/(g1^2*g2^3) + (3*t^8.141)/g2^2 + (3*g1^2*t^8.141)/g2 + (2*g2*t^8.359)/g1^2 + 2*g2^2*t^8.359 + 2*g1^2*g2^3*t^8.359 - (2*t^8.465)/g1 - 2*g1*g2*t^8.465 + 3*g1^2*t^8.57 + (2*t^8.57)/(g1^4*g2^3) + (3*t^8.57)/(g1^2*g2^2) + (2*t^8.57)/g2 + 2*g1^4*g2*t^8.57 + (g2^2*t^8.789)/g1^2 + g2^3*t^8.789 + g1^2*g2^4*t^8.789 + (2*g2*t^8.894)/g1 + 2*g1*g2^2*t^8.894 - t^4.5/y - (g1*t^6.535)/y - t^6.535/(g1*g2*y) + (2*t^7.07)/(g2*y) + (2*t^7.5)/y + t^7.5/(g1^2*g2*y) + (g1^2*g2*t^7.5)/y + (g1*t^8.035)/y + t^8.035/(g1*g2*y) + (4*t^8.465)/(g1*y) + (4*g1*g2*t^8.465)/y + t^8.57/(g2*y) + (3*g2*t^8.894)/(g1*y) + (3*g1*g2^2*t^8.894)/y - t^4.5*y - g1*t^6.535*y - (t^6.535*y)/(g1*g2) + (2*t^7.07*y)/g2 + 2*t^7.5*y + (t^7.5*y)/(g1^2*g2) + g1^2*g2*t^7.5*y + g1*t^8.035*y + (t^8.035*y)/(g1*g2) + (4*t^8.465*y)/g1 + 4*g1*g2*t^8.465*y + (t^8.57*y)/g2 + (3*g2*t^8.894*y)/g1 + 3*g1*g2^2*t^8.894*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 |
|---|---|---|---|---|---|---|---|---|---|
| 103 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6363 | 0.8038 | 0.7916 | [M:[1.142, 0.6775], q:[0.75, 0.4306], qb:[0.4275, 0.392], phi:[0.5]] | t^2.032 + t^2.458 + t^2.468 + t^3. + 2*t^3.426 + t^3.532 + t^3.542 + t^3.852 + t^3.958 + 2*t^4.065 + t^4.074 + t^4.083 + t^4.491 + t^4.5 + t^4.917 + t^4.926 + t^4.935 + t^5.032 + 3*t^5.458 + t^5.468 + t^5.565 + t^5.574 + 2*t^5.884 + t^5.893 + t^5.991 - t^6. - t^4.5/y - t^4.5*y | detail |