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 |
|---|---|---|---|---|---|---|---|---|---|
| 4901 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{3}M_{8}$ | 0.6581 | 0.8183 | 0.8042 | [M:[1.1793, 1.077, 0.9741, 0.8207, 0.8207, 0.7689, 1.077, 1.0259], q:[0.7693, 0.3589], qb:[0.4618, 0.5641], phi:[0.4615]] | [M:[[8], [-4], [10], [-8], [-8], [12], [-4], [-10]], q:[[-1], [3]], qb:[[-11], [1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{8}$, ${ }M_{2}$, ${ }M_{7}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{5}M_{8}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$ | ${}$ | -3 | t^2.307 + 2*t^2.462 + t^3.078 + 2*t^3.231 + t^3.384 + t^3.847 + t^4. + t^4.153 + t^4.155 + t^4.462 + t^4.613 + 3*t^4.769 + 3*t^4.924 + 2*t^5.538 + 2*t^5.54 + 3*t^5.693 + 2*t^5.847 - 3*t^6. + t^6.155 + 3*t^6.309 + t^6.46 + 5*t^6.462 + t^6.616 + 2*t^6.618 - t^6.769 + t^6.92 - t^6.922 + 2*t^6.924 + 2*t^7.076 + t^7.078 + 6*t^7.231 + t^7.233 + 5*t^7.387 + t^7.54 - t^7.691 + 2*t^7.845 + t^7.847 + 3*t^8. + 4*t^8.002 + t^8.153 + 4*t^8.155 - 3*t^8.307 + 3*t^8.309 + t^8.311 - 6*t^8.462 + 3*t^8.618 + t^8.767 + 2*t^8.769 + 4*t^8.771 + t^8.922 + 8*t^8.924 - t^4.384/y - t^6.691/y - t^6.847/y + t^7.153/y - t^7.616/y + (2*t^7.769)/y + t^7.922/y + t^7.924/y + t^8.078/y + t^8.384/y + (2*t^8.538)/y + (2*t^8.54)/y + t^8.691/y + (4*t^8.693)/y + (2*t^8.847)/y - t^8.998/y - t^4.384*y - t^6.691*y - t^6.847*y + t^7.153*y - t^7.616*y + 2*t^7.769*y + t^7.922*y + t^7.924*y + t^8.078*y + t^8.384*y + 2*t^8.538*y + 2*t^8.54*y + t^8.691*y + 4*t^8.693*y + 2*t^8.847*y - t^8.998*y | g1^12*t^2.307 + (2*t^2.462)/g1^8 + t^3.078/g1^10 + (2*t^3.231)/g1^4 + g1^2*t^3.384 + t^3.847/g1^6 + t^4. + g1^6*t^4.153 + t^4.155/g1^20 + t^4.462/g1^8 + g1^24*t^4.613 + 3*g1^4*t^4.769 + (3*t^4.924)/g1^16 + 2*g1^8*t^5.538 + (2*t^5.54)/g1^18 + (3*t^5.693)/g1^12 + (2*t^5.847)/g1^6 - 3*t^6. + t^6.155/g1^20 + (3*t^6.309)/g1^14 + g1^18*t^6.46 + (5*t^6.462)/g1^8 + t^6.616/g1^2 + (2*t^6.618)/g1^28 - g1^4*t^6.769 + g1^36*t^6.92 - g1^10*t^6.922 + (2*t^6.924)/g1^16 + 2*g1^16*t^7.076 + t^7.078/g1^10 + (6*t^7.231)/g1^4 + t^7.233/g1^30 + (5*t^7.387)/g1^24 + t^7.54/g1^18 - g1^14*t^7.691 + 2*g1^20*t^7.845 + t^7.847/g1^6 + 3*t^8. + (4*t^8.002)/g1^26 + g1^6*t^8.153 + (4*t^8.155)/g1^20 - 3*g1^12*t^8.307 + (3*t^8.309)/g1^14 + t^8.311/g1^40 - (6*t^8.462)/g1^8 + (3*t^8.618)/g1^28 + g1^30*t^8.767 + 2*g1^4*t^8.769 + (4*t^8.771)/g1^22 + g1^10*t^8.922 + (8*t^8.924)/g1^16 - (g1^2*t^4.384)/y - (g1^14*t^6.691)/y - t^6.847/(g1^6*y) + (g1^6*t^7.153)/y - t^7.616/(g1^2*y) + (2*g1^4*t^7.769)/y + (g1^10*t^7.922)/y + t^7.924/(g1^16*y) + t^8.078/(g1^10*y) + (g1^2*t^8.384)/y + (2*g1^8*t^8.538)/y + (2*t^8.54)/(g1^18*y) + (g1^14*t^8.691)/y + (4*t^8.693)/(g1^12*y) + (2*t^8.847)/(g1^6*y) - (g1^26*t^8.998)/y - g1^2*t^4.384*y - g1^14*t^6.691*y - (t^6.847*y)/g1^6 + g1^6*t^7.153*y - (t^7.616*y)/g1^2 + 2*g1^4*t^7.769*y + g1^10*t^7.922*y + (t^7.924*y)/g1^16 + (t^8.078*y)/g1^10 + g1^2*t^8.384*y + 2*g1^8*t^8.538*y + (2*t^8.54*y)/g1^18 + g1^14*t^8.691*y + (4*t^8.693*y)/g1^12 + (2*t^8.847*y)/g1^6 - g1^26*t^8.998*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 |
|---|---|---|---|---|---|---|---|---|---|
| 3030 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6618 | 0.823 | 0.8042 | [M:[1.1565, 1.0884, 0.9456, 0.8435, 0.8435, 0.7347, 1.0884], q:[0.7721, 0.3503], qb:[0.4932, 0.5612], phi:[0.4558]] | t^2.204 + 2*t^2.531 + t^2.837 + 2*t^3.265 + t^3.367 + t^3.898 + t^4. + t^4.102 + t^4.327 + t^4.408 + t^4.531 + 3*t^4.735 + t^5.041 + 3*t^5.061 + t^5.367 + 2*t^5.469 + t^5.673 + 3*t^5.796 + 2*t^5.898 - 3*t^6. - t^4.367/y - t^4.367*y | detail |