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 |
|---|---|---|---|---|---|---|---|---|---|
| 6363 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{3}M_{8}$ + ${ }M_{6}M_{8}$ + ${ }M_{9}\phi_{1}^{2}$ | 0.657 | 0.8195 | 0.8017 | [M:[0.8784, 0.7216, 0.7608, 0.8392, 1.1608, 0.7608, 0.8392, 1.2392, 1.2], q:[0.7608, 0.3608], qb:[0.4784, 0.8], phi:[0.4]] | [M:[[2], [-2], [-1], [1], [-1], [-1], [1], [1], [0]], q:[[-1], [-1]], qb:[[2], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{9}$, ${ }M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{7}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{9}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{6}M_{9}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.165 + t^2.282 + 2*t^2.518 + t^2.635 + t^3.365 + t^3.6 + t^3.718 + t^4.07 + t^4.33 + t^4.447 + 2*t^4.565 + 3*t^4.682 + 2*t^4.8 + 2*t^4.918 + 3*t^5.035 + t^5.153 + t^5.27 + t^5.53 + 2*t^5.765 + 3*t^5.882 - 2*t^6. + t^6.118 + 3*t^6.235 + t^6.495 + 2*t^6.588 + t^6.612 + t^6.705 + 3*t^6.73 + 3*t^6.847 + 2*t^6.965 + 4*t^7.082 + 4*t^7.2 + 2*t^7.318 + 4*t^7.435 + 4*t^7.553 + t^7.67 + t^7.695 + 2*t^7.788 + t^7.905 + 3*t^7.93 + 3*t^8.047 + t^8.141 - 3*t^8.165 + t^8.282 + 3*t^8.4 - 5*t^8.518 + t^8.659 + 3*t^8.753 + t^8.777 + 3*t^8.895 + t^8.988 - t^4.2/y - t^6.365/y - t^6.482/y - t^6.718/y - t^6.835/y + t^7.447/y + t^7.565/y + (3*t^7.682)/y + (3*t^7.8)/y + (2*t^7.918)/y + (2*t^8.035)/y + (2*t^8.153)/y + (3*t^8.882)/y - t^4.2*y - t^6.365*y - t^6.482*y - t^6.718*y - t^6.835*y + t^7.447*y + t^7.565*y + 3*t^7.682*y + 3*t^7.8*y + 2*t^7.918*y + 2*t^8.035*y + 2*t^8.153*y + 3*t^8.882*y | t^2.165/g1^2 + t^2.282/g1 + 2*g1*t^2.518 + g1^2*t^2.635 + t^3.365/g1^2 + t^3.6 + g1*t^3.718 + g1^4*t^4.07 + t^4.33/g1^4 + t^4.447/g1^3 + (2*t^4.565)/g1^2 + (3*t^4.682)/g1 + 2*t^4.8 + 2*g1*t^4.918 + 3*g1^2*t^5.035 + g1^3*t^5.153 + g1^4*t^5.27 + t^5.53/g1^4 + (2*t^5.765)/g1^2 + (3*t^5.882)/g1 - 2*t^6. + g1*t^6.118 + 3*g1^2*t^6.235 + t^6.495/g1^6 + 2*g1^5*t^6.588 + t^6.612/g1^5 + g1^6*t^6.705 + (3*t^6.73)/g1^4 + (3*t^6.847)/g1^3 + (2*t^6.965)/g1^2 + (4*t^7.082)/g1 + 4*t^7.2 + 2*g1*t^7.318 + 4*g1^2*t^7.435 + 4*g1^3*t^7.553 + g1^4*t^7.67 + t^7.695/g1^6 + 2*g1^5*t^7.788 + g1^6*t^7.905 + (3*t^7.93)/g1^4 + (3*t^8.047)/g1^3 + g1^8*t^8.141 - (3*t^8.165)/g1^2 + t^8.282/g1 + 3*t^8.4 - 5*g1*t^8.518 + t^8.659/g1^8 + 3*g1^3*t^8.753 + t^8.777/g1^7 + (3*t^8.895)/g1^6 + g1^5*t^8.988 - t^4.2/y - t^6.365/(g1^2*y) - t^6.482/(g1*y) - (g1*t^6.718)/y - (g1^2*t^6.835)/y + t^7.447/(g1^3*y) + t^7.565/(g1^2*y) + (3*t^7.682)/(g1*y) + (3*t^7.8)/y + (2*g1*t^7.918)/y + (2*g1^2*t^8.035)/y + (2*g1^3*t^8.153)/y + (3*t^8.882)/(g1*y) - t^4.2*y - (t^6.365*y)/g1^2 - (t^6.482*y)/g1 - g1*t^6.718*y - g1^2*t^6.835*y + (t^7.447*y)/g1^3 + (t^7.565*y)/g1^2 + (3*t^7.682*y)/g1 + 3*t^7.8*y + 2*g1*t^7.918*y + 2*g1^2*t^8.035*y + 2*g1^3*t^8.153*y + (3*t^8.882*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4759 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{7}$ + ${ }M_{3}M_{8}$ + ${ }M_{6}M_{8}$ | 0.6735 | 0.8485 | 0.7937 | [M:[0.8784, 0.7216, 0.7608, 0.8392, 1.1608, 0.7608, 0.8392, 1.2392], q:[0.7608, 0.3608], qb:[0.4784, 0.8], phi:[0.4]] | t^2.165 + t^2.282 + t^2.4 + 2*t^2.518 + t^2.635 + t^3.365 + t^3.718 + t^4.07 + t^4.33 + t^4.447 + 3*t^4.565 + 4*t^4.682 + 3*t^4.8 + 4*t^4.918 + 4*t^5.035 + t^5.153 + t^5.27 + t^5.53 + 2*t^5.765 + 2*t^5.882 - 2*t^6. - t^4.2/y - t^4.2*y | detail |