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 |
|---|---|---|---|---|---|---|---|---|---|
| 2766 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}q_{2}$ + ${ }M_{3}M_{5}$ | 0.6162 | 0.7743 | 0.7958 | [M:[1.1103, 1.1397, 0.75, 0.7206, 1.25], q:[0.75, 0.5], qb:[0.3897, 0.3603], phi:[0.5]] | [M:[[1], [-1], [0], [2], [0]], q:[[0], [0]], qb:[[-1], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ | ${}M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.162 + t^2.25 + t^3. + 2*t^3.331 + 2*t^3.419 + t^3.662 + 2*t^3.75 + t^4.081 + t^4.169 + t^4.324 + t^4.412 + 2*t^4.5 + t^5.162 + t^5.25 + 2*t^5.493 + 3*t^5.581 + t^5.669 + t^5.824 + 2*t^5.912 - t^6. - t^6.088 + t^6.243 + t^6.331 + t^6.486 + t^6.574 + 5*t^6.662 + 4*t^6.75 + 2*t^6.838 + 2*t^6.993 + 3*t^7.081 + t^7.169 + 2*t^7.324 + 3*t^7.412 + 3*t^7.5 + 2*t^7.655 + 4*t^7.743 + 3*t^7.831 + t^7.919 + t^7.986 + 2*t^8.074 - t^8.25 - t^8.338 + t^8.405 + t^8.493 + t^8.647 + t^8.736 + 5*t^8.824 + 4*t^8.912 - t^4.5/y - t^6.662/y + t^7.081/y + t^7.169/y + t^7.412/y - t^7.831/y - t^7.919/y + t^8.162/y + t^8.25/y + t^8.338/y + (2*t^8.493)/y + (4*t^8.581)/y + (2*t^8.669)/y + (3*t^8.912)/y - t^4.5*y - t^6.662*y + t^7.081*y + t^7.169*y + t^7.412*y - t^7.831*y - t^7.919*y + t^8.162*y + t^8.25*y + t^8.338*y + 2*t^8.493*y + 4*t^8.581*y + 2*t^8.669*y + 3*t^8.912*y | g1^2*t^2.162 + t^2.25 + t^3. + 2*g1*t^3.331 + (2*t^3.419)/g1 + g1^2*t^3.662 + 2*t^3.75 + g1*t^4.081 + t^4.169/g1 + g1^4*t^4.324 + g1^2*t^4.412 + 2*t^4.5 + g1^2*t^5.162 + t^5.25 + 2*g1^3*t^5.493 + 3*g1*t^5.581 + t^5.669/g1 + g1^4*t^5.824 + 2*g1^2*t^5.912 - t^6. - t^6.088/g1^2 + g1^3*t^6.243 + g1*t^6.331 + g1^6*t^6.486 + g1^4*t^6.574 + 5*g1^2*t^6.662 + 4*t^6.75 + (2*t^6.838)/g1^2 + 2*g1^3*t^6.993 + 3*g1*t^7.081 + t^7.169/g1 + 2*g1^4*t^7.324 + 3*g1^2*t^7.412 + 3*t^7.5 + 2*g1^5*t^7.655 + 4*g1^3*t^7.743 + 3*g1*t^7.831 + t^7.919/g1 + g1^6*t^7.986 + 2*g1^4*t^8.074 - t^8.25 - t^8.338/g1^2 + g1^5*t^8.405 + g1^3*t^8.493 + g1^8*t^8.647 + g1^6*t^8.736 + 5*g1^4*t^8.824 + 4*g1^2*t^8.912 - t^4.5/y - (g1^2*t^6.662)/y + (g1*t^7.081)/y + t^7.169/(g1*y) + (g1^2*t^7.412)/y - (g1*t^7.831)/y - t^7.919/(g1*y) + (g1^2*t^8.162)/y + t^8.25/y + t^8.338/(g1^2*y) + (2*g1^3*t^8.493)/y + (4*g1*t^8.581)/y + (2*t^8.669)/(g1*y) + (3*g1^2*t^8.912)/y - t^4.5*y - g1^2*t^6.662*y + g1*t^7.081*y + (t^7.169*y)/g1 + g1^2*t^7.412*y - g1*t^7.831*y - (t^7.919*y)/g1 + g1^2*t^8.162*y + t^8.25*y + (t^8.338*y)/g1^2 + 2*g1^3*t^8.493*y + 4*g1*t^8.581*y + (2*t^8.669*y)/g1 + 3*g1^2*t^8.912*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1761 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}q_{1}q_{2}$ | 0.6352 | 0.809 | 0.7853 | [M:[1.1103, 1.1397, 0.75, 0.7206], q:[0.75, 0.5], qb:[0.3897, 0.3603], phi:[0.5]] | 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^4.5/y - t^4.5*y | detail |