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 |
|---|---|---|---|---|---|---|---|---|---|
| 6278 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{7}$ + ${ }M_{2}X_{1}$ + ${ }M_{1}M_{8}$ + ${ }M_{3}M_{5}$ + ${ }M_{3}M_{9}$ | 0.6798 | 0.8487 | 0.801 | [X:[1.2977], M:[1.1704, 0.7023, 0.9364, 0.9364, 1.0636, 0.8091, 0.8296, 0.8296, 1.0636], q:[0.4784, 0.3511], qb:[0.5852, 0.7125], phi:[0.4682]] | [X:[[6]], M:[[-10], [-6], [-8], [-8], [8], [-24], [10], [10], [8]], q:[[13], [-3]], qb:[[-5], [11]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{7}$, ${ }M_{8}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{9}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{7}M_{8}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{9}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{7}$, ${ }M_{5}M_{8}$, ${ }M_{7}M_{9}$, ${ }M_{8}M_{9}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}M_{4}M_{9}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{9}\phi_{1}^{2}$ | 0 | t^2.427 + 2*t^2.489 + 2*t^2.809 + 2*t^3.191 + 2*t^3.893 + t^4.214 + t^4.275 + 2*t^4.595 + t^4.854 + 2*t^4.916 + 4*t^4.977 + 2*t^5.236 + 3*t^5.298 + 3*t^5.618 + 4*t^5.68 + 4*t^6.382 + t^6.641 + t^6.702 + 2*t^6.764 + 2*t^7.023 + 5*t^7.084 + t^7.282 + 2*t^7.343 + 4*t^7.405 + 6*t^7.466 + 2*t^7.664 + 3*t^7.725 + 5*t^7.786 + 3*t^8.045 + 3*t^8.107 + 7*t^8.168 + t^8.427 - t^8.489 + t^8.55 - 2*t^8.809 + 8*t^8.871 - t^4.405/y - t^6.832/y - t^6.893/y - t^7.214/y + t^7.595/y + (3*t^7.916)/y + (2*t^7.977)/y + (2*t^8.236)/y + (4*t^8.298)/y + (3*t^8.618)/y + (4*t^8.68)/y - t^4.405*y - t^6.832*y - t^6.893*y - t^7.214*y + t^7.595*y + 3*t^7.916*y + 2*t^7.977*y + 2*t^8.236*y + 4*t^8.298*y + 3*t^8.618*y + 4*t^8.68*y | t^2.427/g1^24 + 2*g1^10*t^2.489 + (2*t^2.809)/g1^8 + 2*g1^8*t^3.191 + 2*g1^6*t^3.893 + t^4.214/g1^12 + g1^22*t^4.275 + 2*g1^4*t^4.595 + t^4.854/g1^48 + (2*t^4.916)/g1^14 + 4*g1^20*t^4.977 + (2*t^5.236)/g1^32 + 3*g1^2*t^5.298 + (3*t^5.618)/g1^16 + 4*g1^18*t^5.68 + 4*g1^16*t^6.382 + t^6.641/g1^36 + t^6.702/g1^2 + 2*g1^32*t^6.764 + (2*t^7.023)/g1^20 + 5*g1^14*t^7.084 + t^7.282/g1^72 + (2*t^7.343)/g1^38 + (4*t^7.405)/g1^4 + 6*g1^30*t^7.466 + (2*t^7.664)/g1^56 + (3*t^7.725)/g1^22 + 5*g1^12*t^7.786 + (3*t^8.045)/g1^40 + (3*t^8.107)/g1^6 + 7*g1^28*t^8.168 + t^8.427/g1^24 - g1^10*t^8.489 + g1^44*t^8.55 - (2*t^8.809)/g1^8 + 8*g1^26*t^8.871 - t^4.405/(g1^4*y) - t^6.832/(g1^28*y) - (g1^6*t^6.893)/y - t^7.214/(g1^12*y) + (g1^4*t^7.595)/y + (3*t^7.916)/(g1^14*y) + (2*g1^20*t^7.977)/y + (2*t^8.236)/(g1^32*y) + (4*g1^2*t^8.298)/y + (3*t^8.618)/(g1^16*y) + (4*g1^18*t^8.68)/y - (t^4.405*y)/g1^4 - (t^6.832*y)/g1^28 - g1^6*t^6.893*y - (t^7.214*y)/g1^12 + g1^4*t^7.595*y + (3*t^7.916*y)/g1^14 + 2*g1^20*t^7.977*y + (2*t^8.236*y)/g1^32 + 4*g1^2*t^8.298*y + (3*t^8.618*y)/g1^16 + 4*g1^18*t^8.68*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4713 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{7}$ + ${ }M_{2}X_{1}$ + ${ }M_{1}M_{8}$ + ${ }M_{3}M_{5}$ | 0.6861 | 0.8591 | 0.7986 | [X:[1.3036], M:[1.1607, 0.6964, 0.9285, 0.9285, 1.0715, 0.7856, 0.8393, 0.8393], q:[0.4911, 0.3482], qb:[0.5803, 0.7233], phi:[0.4643]] | t^2.357 + 2*t^2.518 + 3*t^2.786 + t^3.214 + 2*t^3.911 + t^4.178 + t^4.34 + 2*t^4.607 + t^4.714 + 2*t^4.875 + 4*t^5.036 + 3*t^5.142 + 5*t^5.304 + 5*t^5.571 + 2*t^5.732 - t^6. - t^4.393/y - t^4.393*y | detail |