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 |
|---|---|---|---|---|---|---|---|---|---|
| 60549 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{2}\tilde{q}_{1}X_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{2}$ | 1.0815 | 1.2564 | 0.8608 | [X:[1.6011, 1.3933], M:[1.2022, 0.9944], q:[0.7355, 0.1344], qb:[0.2645, 0.4724], phi:[0.3989]] | [X:[[0, -1], [0, 6]], M:[[0, -2], [0, 5]], q:[[-1, -7], [-1, -6]], qb:[[1, 7], [1, 0]], phi:[[0, 1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}\phi_{1}^{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }\phi_{1}^{5}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}q_{2}\tilde{q}_{1}$ | ${}$ | -4 | t^2.39 + t^2.98 + t^3. + 2*t^3.59 + t^3.61 + t^3.62 + t^4.18 + t^4.2 + 2*t^4.21 + t^4.79 + 2*t^4.8 + 2*t^4.82 + t^5.39 + t^5.4 + t^5.41 + 2*t^5.97 + 3*t^5.98 - 4*t^6. + t^6.01 + 3*t^6.02 + 2*t^6.57 - t^6.58 + 3*t^6.59 + 2*t^6.6 + 3*t^6.61 - t^6.62 + t^7.16 + 6*t^7.18 + t^7.19 - t^7.2 + 4*t^7.21 + t^7.22 + t^7.23 + t^7.25 + 5*t^7.79 + 6*t^7.8 + t^7.83 + 2*t^7.84 + 2*t^8.36 + 4*t^8.38 - t^8.39 + 7*t^8.41 + 2*t^8.42 + 2*t^8.43 + t^8.44 + t^8.45 + 2*t^8.95 - 3*t^8.98 + 2*t^8.99 - t^4.2/y - t^5.39/y - t^7.18/y - t^7.2/y + t^7.21/y - (2*t^7.79)/y - t^7.82/y - t^8.38/y + t^8.39/y + (2*t^8.98)/y - t^4.2*y - t^5.39*y - t^7.18*y - t^7.2*y + t^7.21*y - 2*t^7.79*y - t^7.82*y - t^8.38*y + t^8.39*y + 2*t^8.98*y | g2^2*t^2.39 + g2^5*t^2.98 + t^3. + 2*g2^3*t^3.59 + t^3.61/g2^2 + t^3.62/g2^7 + g2^6*t^4.18 + g1^3*g2^15*t^4.2 + t^4.21/(g1^3*g2^18) + t^4.21/g2^4 + g2^4*t^4.79 + t^4.8/(g1^3*g2^15) + t^4.8/g2 + t^4.82/g2^6 + g1^3*g2^8*t^4.82 + g2^2*t^5.39 + g1^3*g2^16*t^5.4 + t^5.41/(g1^3*g2^17) + g2^10*t^5.97 + g1^3*g2^24*t^5.97 + 3*g2^5*t^5.98 - 3*t^6. - g1^3*g2^14*t^6. + t^6.01/(g1^3*g2^19) + (2*t^6.02)/g2^5 + g1^3*g2^9*t^6.02 + 2*g2^8*t^6.57 - g1^3*g2^22*t^6.58 - t^6.59/(g1^3*g2^11) + 2*g2^3*t^6.59 + 2*g1^3*g2^17*t^6.59 + (2*t^6.6)/(g1^3*g2^16) + (3*t^6.61)/g2^2 - t^6.62/g2^7 + g2^11*t^7.16 + 5*g2^6*t^7.18 + g1^3*g2^20*t^7.18 + t^7.19/(g1^3*g2^13) - g1^3*g2^15*t^7.2 + (4*t^7.21)/g2^4 + g1^3*g2^10*t^7.22 + t^7.23/g2^9 + t^7.25/g2^14 + g2^9*t^7.77 - g1^3*g2^23*t^7.77 + 3*g2^4*t^7.79 + 2*g1^3*g2^18*t^7.79 + (3*t^7.8)/(g1^3*g2^15) + (3*t^7.8)/g2 - t^7.82/(g1^3*g2^20) + g1^3*g2^8*t^7.82 + t^7.83/(g1^3*g2^25) + t^7.84/g2^11 + g1^3*g2^3*t^7.84 + g2^12*t^8.36 + g1^3*g2^26*t^8.36 + 3*g2^7*t^8.38 + g1^3*g2^21*t^8.38 + (2*t^8.39)/(g1^3*g2^12) - 3*g2^2*t^8.39 - g1^3*g2^16*t^8.4 + g1^6*g2^30*t^8.4 + t^8.41/(g1^3*g2^17) + (4*t^8.41)/g2^3 + 2*g1^3*g2^11*t^8.41 + t^8.42/(g1^6*g2^36) + t^8.42/(g1^3*g2^22) + (2*t^8.43)/g2^8 + t^8.44/g2^13 + g1^3*g2*t^8.45 + g2^15*t^8.95 + g1^3*g2^29*t^8.95 + g2^10*t^8.97 - g1^3*g2^24*t^8.97 - t^8.98/(g1^3*g2^9) - 2*g2^5*t^8.98 + 2*g1^3*g2^19*t^8.99 - (g2*t^4.2)/y - (g2^2*t^5.39)/y - (g2^6*t^7.18)/y - (g2*t^7.2)/y + t^7.21/(g2^4*y) - (2*g2^4*t^7.79)/y - t^7.82/(g2^6*y) - (g2^7*t^8.38)/y + (g2^2*t^8.39)/y + (2*g2^5*t^8.98)/y - g2*t^4.2*y - g2^2*t^5.39*y - g2^6*t^7.18*y - g2*t^7.2*y + (t^7.21*y)/g2^4 - 2*g2^4*t^7.79*y - (t^7.82*y)/g2^6 - g2^7*t^8.38*y + g2^2*t^8.39*y + 2*g2^5*t^8.98*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57419 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.5158 | 1.7662 | 0.8582 | [M:[0.6699, 0.6766], q:[0.4996, 0.4944], qb:[0.5004, 0.4937], phi:[0.3353]] | t^2.01 + t^2.012 + t^2.03 + t^2.964 + t^2.98 + t^2.984 + t^3. + t^3.018 + t^3.986 + t^4.006 + t^4.02 + t^4.022 + t^4.024 + t^4.04 + t^4.042 + t^4.06 + t^4.974 + 2*t^4.976 + t^4.99 + 2*t^4.992 + 2*t^4.994 + 2*t^4.996 + 2*t^5.01 + 2*t^5.012 + t^5.014 + t^5.028 + 2*t^5.03 + t^5.048 + t^5.469 + t^5.471 + t^5.487 + t^5.489 + t^5.928 + t^5.944 + t^5.948 + t^5.96 + 2*t^5.964 + t^5.968 + t^5.982 + t^5.996 + 2*t^5.998 - 3*t^6. - t^4.006/y - t^5.012/y - t^4.006*y - t^5.012*y | detail |