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 |
|---|---|---|---|---|---|---|---|---|---|
| 6926 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{8}$ + ${ }M_{7}^{2}$ + ${ }M_{4}X_{1}$ | 0.6234 | 0.7874 | 0.7916 | [X:[1.4167], M:[0.75, 1.0833, 1.25, 0.5833, 0.7917, 0.875, 1.0, 0.9167], q:[0.4792, 0.7708], qb:[0.2708, 0.6458], phi:[0.4583]] | [X:[[0]], M:[[0], [0], [0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 10213/16384, c: 12901/16384, X1: 17/12, M1: 3/4, M2: 13/12, M3: 5/4, M4: 7/12, M5: 19/24, M6: 7/8, M7: 1, M8: 11/12, q1: 23/48, q2: 37/48, qb1: 13/48, qb2: 31/48, phi1: 11/24} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{7}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{8}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | ${}$ | -1 | t^2.25 + t^2.375 + t^2.625 + 2*t^2.75 + t^3. + t^3.125 + t^3.75 + t^4.125 + 2*t^4.25 + t^4.5 + t^4.625 + 2*t^4.75 + 3*t^5. + 2*t^5.125 + 3*t^5.25 + 3*t^5.375 + 3*t^5.5 + t^5.625 + 3*t^5.75 + t^5.875 - t^6. + 2*t^6.125 - t^6.25 + 2*t^6.5 + t^6.625 + t^6.75 + 3*t^6.875 + 4*t^7. + 2*t^7.125 + 3*t^7.25 + 2*t^7.375 + 4*t^7.5 + 3*t^7.625 + 4*t^7.75 + 4*t^7.875 + 6*t^8. + 5*t^8.125 + 4*t^8.25 + 2*t^8.375 + 5*t^8.5 - 2*t^8.625 - 2*t^8.75 - t^4.375/y - t^6.75/y - t^7./y - t^7.125/y + (2*t^7.625)/y + t^7.75/y + t^7.875/y + (4*t^8.)/y + (2*t^8.125)/y + t^8.25/y + (4*t^8.375)/y + (2*t^8.5)/y + t^8.625/y + (3*t^8.75)/y + (2*t^8.875)/y - t^4.375*y - t^6.75*y - t^7.*y - t^7.125*y + 2*t^7.625*y + t^7.75*y + t^7.875*y + 4*t^8.*y + 2*t^8.125*y + t^8.25*y + 4*t^8.375*y + 2*t^8.5*y + t^8.625*y + 3*t^8.75*y + 2*t^8.875*y | t^2.25 + t^2.375 + t^2.625 + 2*t^2.75 + t^3. + t^3.125 + t^3.75 + t^4.125 + 2*t^4.25 + t^4.5 + t^4.625 + 2*t^4.75 + 3*t^5. + 2*t^5.125 + 3*t^5.25 + 3*t^5.375 + 3*t^5.5 + t^5.625 + 3*t^5.75 + t^5.875 - t^6. + 2*t^6.125 - t^6.25 + 2*t^6.5 + t^6.625 + t^6.75 + 3*t^6.875 + 4*t^7. + 2*t^7.125 + 3*t^7.25 + 2*t^7.375 + 4*t^7.5 + 3*t^7.625 + 4*t^7.75 + 4*t^7.875 + 6*t^8. + 5*t^8.125 + 4*t^8.25 + 2*t^8.375 + 5*t^8.5 - 2*t^8.625 - 2*t^8.75 - t^4.375/y - t^6.75/y - t^7./y - t^7.125/y + (2*t^7.625)/y + t^7.75/y + t^7.875/y + (4*t^8.)/y + (2*t^8.125)/y + t^8.25/y + (4*t^8.375)/y + (2*t^8.5)/y + t^8.625/y + (3*t^8.75)/y + (2*t^8.875)/y - t^4.375*y - t^6.75*y - t^7.*y - t^7.125*y + 2*t^7.625*y + t^7.75*y + t^7.875*y + 4*t^8.*y + 2*t^8.125*y + t^8.25*y + 4*t^8.375*y + 2*t^8.5*y + t^8.625*y + 3*t^8.75*y + 2*t^8.875*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 |
|---|---|---|---|---|---|---|---|---|---|
| 5483 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{8}$ | 0.7 | 0.8987 | 0.7789 | [M:[0.8247, 1.0584, 1.1753, 0.7078, 0.7045, 1.0618, 0.7012, 0.9416], q:[0.4107, 0.7646], qb:[0.414, 0.5276], phi:[0.4708]] | t^2.104 + t^2.114 + t^2.124 + t^2.474 + 2*t^2.825 + t^3.185 + t^3.526 + t^3.536 + t^3.876 + t^4.207 + t^4.217 + 3*t^4.227 + 2*t^4.237 + t^4.247 + 2*t^4.578 + t^4.588 + t^4.598 + 2*t^4.928 + 2*t^4.938 + 3*t^4.948 + t^5.289 + 3*t^5.299 + t^5.309 + t^5.629 + 2*t^5.639 + 4*t^5.649 + t^5.659 + t^5.98 - t^6. - t^4.412/y - t^4.412*y | detail |