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 |
|---|---|---|---|---|---|---|---|---|---|
| 50912 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ | 0.6707 | 0.8463 | 0.7925 | [M:[1.1449, 0.7174, 0.8551, 0.8092, 0.8092, 0.7633], q:[0.4046, 0.4505], qb:[0.878, 0.7404], phi:[0.3816]] | [M:[[12], [18], [-12], [-2], [-2], [8]], q:[[-1], [-11]], qb:[[-17], [13]], phi:[[4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}\phi_{1}^{2}$ | ${}$ | -1 | t^2.152 + 2*t^2.29 + 2*t^2.428 + t^2.565 + t^3.435 + t^3.848 + t^3.985 + t^4.304 + 2*t^4.442 + 5*t^4.58 + 5*t^4.717 + 6*t^4.855 + 2*t^4.993 + t^5.13 + t^5.587 + t^5.725 - t^6. + t^6.138 + 3*t^6.275 + 3*t^6.413 + t^6.457 + t^6.551 + 2*t^6.594 + 5*t^6.732 + 9*t^6.87 + 10*t^7.007 + 10*t^7.145 + 8*t^7.283 + 3*t^7.42 + t^7.696 + t^7.739 + t^7.833 + t^7.877 + t^7.971 + t^8.015 - 3*t^8.152 - 4*t^8.29 - 6*t^8.428 + t^8.609 + 5*t^8.703 + 2*t^8.747 + 6*t^8.84 + 5*t^8.884 + 3*t^8.978 - t^4.145/y - t^6.297/y - (2*t^6.435)/y - (2*t^6.572)/y + (2*t^7.442)/y + (3*t^7.58)/y + (7*t^7.717)/y + (5*t^7.855)/y + (3*t^7.993)/y - t^8.449/y - t^8.587/y - (3*t^8.725)/y - (2*t^8.862)/y - t^4.145*y - t^6.297*y - 2*t^6.435*y - 2*t^6.572*y + 2*t^7.442*y + 3*t^7.58*y + 7*t^7.717*y + 5*t^7.855*y + 3*t^7.993*y - t^8.449*y - t^8.587*y - 3*t^8.725*y - 2*t^8.862*y | g1^18*t^2.152 + 2*g1^8*t^2.29 + (2*t^2.428)/g1^2 + t^2.565/g1^12 + g1^12*t^3.435 + t^3.848/g1^18 + t^3.985/g1^28 + g1^36*t^4.304 + 2*g1^26*t^4.442 + 5*g1^16*t^4.58 + 5*g1^6*t^4.717 + (6*t^4.855)/g1^4 + (2*t^4.993)/g1^14 + t^5.13/g1^24 + g1^30*t^5.587 + g1^20*t^5.725 - t^6. + t^6.138/g1^10 + (3*t^6.275)/g1^20 + (3*t^6.413)/g1^30 + g1^54*t^6.457 + t^6.551/g1^40 + 2*g1^44*t^6.594 + 5*g1^34*t^6.732 + 9*g1^24*t^6.87 + 10*g1^14*t^7.007 + 10*g1^4*t^7.145 + (8*t^7.283)/g1^6 + (3*t^7.42)/g1^16 + t^7.696/g1^36 + g1^48*t^7.739 + t^7.833/g1^46 + g1^38*t^7.877 + t^7.971/g1^56 + g1^28*t^8.015 - 3*g1^18*t^8.152 - 4*g1^8*t^8.29 - (6*t^8.428)/g1^2 + g1^72*t^8.609 + (5*t^8.703)/g1^22 + 2*g1^62*t^8.747 + (6*t^8.84)/g1^32 + 5*g1^52*t^8.884 + (3*t^8.978)/g1^42 - (g1^4*t^4.145)/y - (g1^22*t^6.297)/y - (2*g1^12*t^6.435)/y - (2*g1^2*t^6.572)/y + (2*g1^26*t^7.442)/y + (3*g1^16*t^7.58)/y + (7*g1^6*t^7.717)/y + (5*t^7.855)/(g1^4*y) + (3*t^7.993)/(g1^14*y) - (g1^40*t^8.449)/y - (g1^30*t^8.587)/y - (3*g1^20*t^8.725)/y - (2*g1^10*t^8.862)/y - g1^4*t^4.145*y - g1^22*t^6.297*y - 2*g1^12*t^6.435*y - 2*g1^2*t^6.572*y + 2*g1^26*t^7.442*y + 3*g1^16*t^7.58*y + 7*g1^6*t^7.717*y + (5*t^7.855*y)/g1^4 + (3*t^7.993*y)/g1^14 - g1^40*t^8.449*y - g1^30*t^8.587*y - 3*g1^20*t^8.725*y - 2*g1^10*t^8.862*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 |
|---|---|---|---|---|---|---|---|---|---|
| 48251 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ | 0.6708 | 0.8471 | 0.7919 | [M:[1.1466, 0.7084, 0.8534, 0.8203, 0.7975, 0.7644], q:[0.4101, 0.4433], qb:[0.8814, 0.7364], phi:[0.3822]] | t^2.125 + 2*t^2.293 + t^2.393 + t^2.461 + t^2.56 + t^3.44 + t^3.806 + t^3.974 + t^4.251 + 2*t^4.418 + t^4.518 + 4*t^4.586 + 3*t^4.686 + 2*t^4.754 + t^4.785 + 4*t^4.853 + t^4.922 + t^4.953 + t^5.021 + t^5.121 + t^5.565 + t^5.733 + t^5.932 - 2*t^6. - t^4.147/y - t^4.147*y | detail |