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 |
|---|---|---|---|---|---|---|---|---|---|
| 46487 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ | 0.6352 | 0.809 | 0.7853 | [M:[1.1397, 0.75, 0.7206, 1.1103], q:[0.75, 0.3603], qb:[0.3897, 0.5], phi:[0.5]] | [M:[[1], [0], [-2], [-1]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }q_{1}q_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}^{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | ${}$ | -1 | t^2.162 + 2*t^2.25 + t^3. + 2*t^3.331 + 2*t^3.419 + t^3.662 + t^3.75 + t^4.081 + t^4.169 + t^4.324 + 2*t^4.412 + 4*t^4.5 + t^5.162 + 2*t^5.25 + 2*t^5.493 + 5*t^5.581 + 3*t^5.669 + t^5.824 + 2*t^5.912 - t^6. - t^6.088 + t^6.243 + 2*t^6.331 + t^6.419 + t^6.486 + 2*t^6.574 + 7*t^6.662 + 7*t^6.75 + 2*t^6.838 + 2*t^6.993 + t^7.081 - t^7.169 + 2*t^7.324 + 3*t^7.412 + 3*t^7.5 + 2*t^7.655 + 6*t^7.743 + 7*t^7.831 + 3*t^7.919 + t^7.986 + 2*t^8.074 + t^8.162 - 4*t^8.25 - 2*t^8.338 + t^8.405 + 2*t^8.493 + 2*t^8.581 + t^8.647 + t^8.669 + 2*t^8.736 + 7*t^8.824 + 10*t^8.912 - t^4.5/y - t^6.662/y - t^6.75/y + t^7.081/y + t^7.169/y + (2*t^7.412)/y + t^7.5/y - t^7.831/y - t^7.919/y + t^8.162/y + (3*t^8.25)/y + t^8.338/y + (2*t^8.493)/y + (6*t^8.581)/y + (4*t^8.669)/y + (2*t^8.912)/y - t^4.5*y - t^6.662*y - t^6.75*y + t^7.081*y + t^7.169*y + 2*t^7.412*y + t^7.5*y - t^7.831*y - t^7.919*y + t^8.162*y + 3*t^8.25*y + t^8.338*y + 2*t^8.493*y + 6*t^8.581*y + 4*t^8.669*y + 2*t^8.912*y | t^2.162/g1^2 + 2*t^2.25 + t^3. + (2*t^3.331)/g1 + 2*g1*t^3.419 + t^3.662/g1^2 + t^3.75 + t^4.081/g1 + g1*t^4.169 + t^4.324/g1^4 + (2*t^4.412)/g1^2 + 4*t^4.5 + t^5.162/g1^2 + 2*t^5.25 + (2*t^5.493)/g1^3 + (5*t^5.581)/g1 + 3*g1*t^5.669 + t^5.824/g1^4 + (2*t^5.912)/g1^2 - t^6. - g1^2*t^6.088 + t^6.243/g1^3 + (2*t^6.331)/g1 + g1*t^6.419 + t^6.486/g1^6 + (2*t^6.574)/g1^4 + (7*t^6.662)/g1^2 + 7*t^6.75 + 2*g1^2*t^6.838 + (2*t^6.993)/g1^3 + t^7.081/g1 - g1*t^7.169 + (2*t^7.324)/g1^4 + (3*t^7.412)/g1^2 + 3*t^7.5 + (2*t^7.655)/g1^5 + (6*t^7.743)/g1^3 + (7*t^7.831)/g1 + 3*g1*t^7.919 + t^7.986/g1^6 + (2*t^8.074)/g1^4 + t^8.162/g1^2 - 4*t^8.25 - 2*g1^2*t^8.338 + t^8.405/g1^5 + (2*t^8.493)/g1^3 + (2*t^8.581)/g1 + t^8.647/g1^8 + g1*t^8.669 + (2*t^8.736)/g1^6 + (7*t^8.824)/g1^4 + (10*t^8.912)/g1^2 - t^4.5/y - t^6.662/(g1^2*y) - t^6.75/y + t^7.081/(g1*y) + (g1*t^7.169)/y + (2*t^7.412)/(g1^2*y) + t^7.5/y - t^7.831/(g1*y) - (g1*t^7.919)/y + t^8.162/(g1^2*y) + (3*t^8.25)/y + (g1^2*t^8.338)/y + (2*t^8.493)/(g1^3*y) + (6*t^8.581)/(g1*y) + (4*g1*t^8.669)/y + (2*t^8.912)/(g1^2*y) - t^4.5*y - (t^6.662*y)/g1^2 - t^6.75*y + (t^7.081*y)/g1 + g1*t^7.169*y + (2*t^7.412*y)/g1^2 + t^7.5*y - (t^7.831*y)/g1 - g1*t^7.919*y + (t^8.162*y)/g1^2 + 3*t^8.25*y + g1^2*t^8.338*y + (2*t^8.493*y)/g1^3 + (6*t^8.581*y)/g1 + 4*g1*t^8.669*y + (2*t^8.912*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46201 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6426 | 0.819 | 0.7847 | [M:[1.1608, 0.6858, 0.6783, 1.1534], q:[0.75, 0.4034], qb:[0.4108, 0.4358], phi:[0.5]] | t^2.035 + t^2.057 + t^2.443 + t^3. + 2*t^3.46 + 2*t^3.482 + t^3.557 + t^3.92 + t^4.018 + t^4.04 + t^4.07 + t^4.092 + 2*t^4.115 + t^4.478 + t^4.5 + t^4.885 + t^5.035 + t^5.057 + t^5.443 + 2*t^5.495 + 4*t^5.518 + 2*t^5.54 + t^5.592 + t^5.615 + t^5.903 + t^5.925 + t^5.955 - 2*t^6. - t^4.5/y - t^4.5*y | detail |