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 |
|---|---|---|---|---|---|---|---|---|---|
| 1677 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ | 0.6468 | 0.8098 | 0.7987 | [M:[0.8085, 1.2, 0.7915, 0.8, 1.1915, 0.8169, 0.7831], q:[0.8, 0.3915], qb:[0.8, 0.4085], phi:[0.4]] | [M:[[1], [0], [-1], [0], [-1], [2], [-2]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{3}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{5}$, ${ }q_{1}q_{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}q_{1}q_{2}$, ${ }M_{3}M_{5}$, ${ }M_{2}M_{7}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{2}M_{3}$, ${ }M_{4}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{7}q_{1}\tilde{q}_{2}$ | ${}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | 0 | t^2.349 + t^2.375 + 2*t^2.4 + t^2.451 + 2*t^3.575 + t^3.6 + t^3.625 + t^4.699 + t^4.724 + 3*t^4.749 + 2*t^4.775 + 5*t^4.8 + t^4.825 + 2*t^4.851 + t^4.901 + 2*t^5.924 + 2*t^5.949 + 4*t^5.975 + 2*t^6.025 + t^6.076 + t^7.048 + t^7.073 + 3*t^7.099 + 3*t^7.124 + 8*t^7.149 + 3*t^7.175 + 7*t^7.2 - t^7.225 + 4*t^7.251 + t^7.276 + 2*t^7.301 + t^7.352 + 2*t^8.273 + 2*t^8.299 + 5*t^8.324 + 4*t^8.375 - 2*t^8.4 + t^8.425 - 3*t^8.451 + 2*t^8.476 + t^8.527 - t^4.2/y - t^6.549/y - t^6.575/y - t^6.6/y - t^6.651/y + t^7.724/y + (3*t^7.749)/y + (2*t^7.775)/y + (3*t^7.8)/y + (2*t^7.825)/y + (3*t^7.851)/y - t^8.899/y + t^8.924/y + t^8.949/y + (5*t^8.975)/y - t^4.2*y - t^6.549*y - t^6.575*y - t^6.6*y - t^6.651*y + t^7.724*y + 3*t^7.749*y + 2*t^7.775*y + 3*t^7.8*y + 2*t^7.825*y + 3*t^7.851*y - t^8.899*y + t^8.924*y + t^8.949*y + 5*t^8.975*y | t^2.349/g1^2 + t^2.375/g1 + 2*t^2.4 + g1^2*t^2.451 + (2*t^3.575)/g1 + t^3.6 + g1*t^3.625 + t^4.699/g1^4 + t^4.724/g1^3 + (3*t^4.749)/g1^2 + (2*t^4.775)/g1 + 5*t^4.8 + g1*t^4.825 + 2*g1^2*t^4.851 + g1^4*t^4.901 + (2*t^5.924)/g1^3 + (2*t^5.949)/g1^2 + (4*t^5.975)/g1 + 2*g1*t^6.025 + g1^3*t^6.076 + t^7.048/g1^6 + t^7.073/g1^5 + (3*t^7.099)/g1^4 + (3*t^7.124)/g1^3 + (8*t^7.149)/g1^2 + (3*t^7.175)/g1 + 7*t^7.2 - g1*t^7.225 + 4*g1^2*t^7.251 + g1^3*t^7.276 + 2*g1^4*t^7.301 + g1^6*t^7.352 + (2*t^8.273)/g1^5 + (2*t^8.299)/g1^4 + (5*t^8.324)/g1^3 + (4*t^8.375)/g1 - 2*t^8.4 + g1*t^8.425 - 3*g1^2*t^8.451 + 2*g1^3*t^8.476 + g1^5*t^8.527 - t^4.2/y - t^6.549/(g1^2*y) - t^6.575/(g1*y) - t^6.6/y - (g1^2*t^6.651)/y + t^7.724/(g1^3*y) + (3*t^7.749)/(g1^2*y) + (2*t^7.775)/(g1*y) + (3*t^7.8)/y + (2*g1*t^7.825)/y + (3*g1^2*t^7.851)/y - t^8.899/(g1^4*y) + t^8.924/(g1^3*y) + t^8.949/(g1^2*y) + (5*t^8.975)/(g1*y) - t^4.2*y - (t^6.549*y)/g1^2 - (t^6.575*y)/g1 - t^6.6*y - g1^2*t^6.651*y + (t^7.724*y)/g1^3 + (3*t^7.749*y)/g1^2 + (2*t^7.775*y)/g1 + 3*t^7.8*y + 2*g1*t^7.825*y + 3*g1^2*t^7.851*y - (t^8.899*y)/g1^4 + (t^8.924*y)/g1^3 + (t^8.949*y)/g1^2 + (5*t^8.975*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 |
|---|---|---|---|---|---|---|---|---|---|
| 1078 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6303 | 0.781 | 0.8071 | [M:[0.7897, 1.2, 0.8103, 0.8, 1.2103, 0.7793], q:[0.8, 0.4103], qb:[0.8, 0.3897], phi:[0.4]] | t^2.338 + 2*t^2.4 + t^2.431 + t^3.538 + t^3.569 + t^3.6 + 2*t^3.631 + t^4.676 + 2*t^4.738 + t^4.769 + 4*t^4.8 + 2*t^4.831 + t^4.862 + t^5.876 + t^5.907 + 2*t^5.938 + 3*t^5.969 - t^4.2/y - t^4.2*y | detail |