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 |
|---|---|---|---|---|---|---|---|---|---|
| 3851 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6338 | 0.781 | 0.8115 | [X:[1.6128], M:[0.8383, 0.7107, 1.1617, 0.3872, 0.8383, 0.7426, 1.2893], q:[0.4032, 0.7585], qb:[0.4351, 0.8542], phi:[0.3872]] | [X:[[4]], M:[[12], [-28], [-12], [-4], [12], [-18], [28]], q:[[1], [-13]], qb:[[11], [17]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{7}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}^{2}$, ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | ${}\phi_{1}^{3}q_{1}\tilde{q}_{1}$ | -1 | t^2.228 + t^2.323 + 2*t^2.515 + 2*t^3.581 + t^3.677 + t^3.772 + t^3.868 + t^4.456 + t^4.551 + t^4.647 + 2*t^4.743 + 3*t^4.838 + 3*t^5.03 + t^5.809 + t^5.904 - t^6. + 4*t^6.096 + 2*t^6.191 + 2*t^6.287 + 2*t^6.383 + t^6.683 + t^6.779 + t^6.875 + 2*t^6.97 + t^7.066 + 3*t^7.162 + t^7.257 + 4*t^7.353 + t^7.449 + 5*t^7.544 + t^7.64 + t^7.736 + t^8.036 - t^8.228 + t^8.419 - 3*t^8.515 + 5*t^8.61 + 3*t^8.706 + 3*t^8.802 + 3*t^8.898 + t^8.911 - t^4.162/y - t^6.39/y - t^6.485/y - t^6.677/y + t^7.551/y + t^7.647/y + (2*t^7.743)/y + (3*t^7.838)/y + t^7.934/y + t^8.03/y - t^8.617/y - t^8.713/y + t^8.809/y + (2*t^8.904)/y - t^4.162*y - t^6.39*y - t^6.485*y - t^6.677*y + t^7.551*y + t^7.647*y + 2*t^7.743*y + 3*t^7.838*y + t^7.934*y + t^8.03*y - t^8.617*y - t^8.713*y + t^8.809*y + 2*t^8.904*y | t^2.228/g1^18 + t^2.323/g1^8 + 2*g1^12*t^2.515 + (2*t^3.581)/g1^2 + g1^8*t^3.677 + g1^18*t^3.772 + g1^28*t^3.868 + t^4.456/g1^36 + t^4.551/g1^26 + t^4.647/g1^16 + (2*t^4.743)/g1^6 + 3*g1^4*t^4.838 + 3*g1^24*t^5.03 + t^5.809/g1^20 + t^5.904/g1^10 - t^6. + 4*g1^10*t^6.096 + 2*g1^20*t^6.191 + 2*g1^30*t^6.287 + 2*g1^40*t^6.383 + t^6.683/g1^54 + t^6.779/g1^44 + t^6.875/g1^34 + (2*t^6.97)/g1^24 + t^7.066/g1^14 + (3*t^7.162)/g1^4 + g1^6*t^7.257 + 4*g1^16*t^7.353 + g1^26*t^7.449 + 5*g1^36*t^7.544 + g1^46*t^7.64 + g1^56*t^7.736 + t^8.036/g1^38 - t^8.228/g1^18 + g1^2*t^8.419 - 3*g1^12*t^8.515 + 5*g1^22*t^8.61 + 3*g1^32*t^8.706 + 3*g1^42*t^8.802 + 3*g1^52*t^8.898 + t^8.911/g1^72 - t^4.162/(g1^4*y) - t^6.39/(g1^22*y) - t^6.485/(g1^12*y) - (g1^8*t^6.677)/y + t^7.551/(g1^26*y) + t^7.647/(g1^16*y) + (2*t^7.743)/(g1^6*y) + (3*g1^4*t^7.838)/y + (g1^14*t^7.934)/y + (g1^24*t^8.03)/y - t^8.617/(g1^40*y) - t^8.713/(g1^30*y) + t^8.809/(g1^20*y) + (2*t^8.904)/(g1^10*y) - (t^4.162*y)/g1^4 - (t^6.39*y)/g1^22 - (t^6.485*y)/g1^12 - g1^8*t^6.677*y + (t^7.551*y)/g1^26 + (t^7.647*y)/g1^16 + (2*t^7.743*y)/g1^6 + 3*g1^4*t^7.838*y + g1^14*t^7.934*y + g1^24*t^8.03*y - (t^8.617*y)/g1^40 - (t^8.713*y)/g1^30 + (t^8.809*y)/g1^20 + (2*t^8.904*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3377 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{7}$ | 0.6342 | 0.7831 | 0.8099 | [X:[1.6118], M:[0.8354, 0.7174, 1.1646, 0.3882, 0.8354, 0.7243, 1.2826], q:[0.3916, 0.773], qb:[0.4437, 0.8388], phi:[0.3882]] | t^2.173 + t^2.329 + 2*t^2.506 + t^3.514 + t^3.65 + t^3.671 + t^3.691 + t^3.848 + t^4.346 + t^4.502 + t^4.658 + 2*t^4.679 + 3*t^4.835 + 3*t^5.012 + t^5.687 + t^5.844 + t^5.864 - 2*t^6. - t^4.165/y - t^4.165*y | detail |