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 |
|---|---|---|---|---|---|---|---|---|---|
| 46562 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ | 0.6784 | 0.8379 | 0.8097 | [M:[1.104, 0.688, 1.104, 0.792], q:[0.464, 0.432], qb:[0.776, 0.536], phi:[0.448]] | [M:[[4], [-12], [4], [-8]], q:[[-11], [7]], qb:[[1], [11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{3}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}M_{2}\phi_{1}q_{2}^{2}$ | -1 | t^2.064 + t^2.376 + t^2.904 + t^3. + 2*t^3.312 + t^3.72 + t^3.936 + t^4.032 + 2*t^4.128 + t^4.248 + t^4.344 + t^4.44 + t^4.56 + t^4.752 + t^4.968 + t^5.064 + t^5.28 + 3*t^5.376 + t^5.688 + t^5.808 - t^6. + t^6.096 + 2*t^6.192 + t^6.216 + 2*t^6.312 + t^6.408 + 2*t^6.504 + 4*t^6.624 + t^6.72 + t^6.816 + t^6.84 + t^6.936 + 2*t^7.032 + 2*t^7.128 + t^7.152 + t^7.248 + t^7.344 + 4*t^7.44 + t^7.464 + t^7.56 + t^7.656 + 2*t^7.752 + t^7.848 + 2*t^7.872 + t^8.064 + t^8.16 + t^8.184 + 3*t^8.256 + t^8.28 + 2*t^8.472 + t^8.496 + 2*t^8.568 + 4*t^8.688 + t^8.712 + t^8.784 + t^8.808 + 2*t^8.88 - t^8.904 - t^4.344/y - t^6.408/y - t^6.72/y + t^7.032/y + t^7.44/y - t^7.656/y + (2*t^7.968)/y + t^8.064/y + (2*t^8.28)/y + (3*t^8.376)/y - t^8.472/y + (2*t^8.688)/y + t^8.904/y - t^4.344*y - t^6.408*y - t^6.72*y + t^7.032*y + t^7.44*y - t^7.656*y + 2*t^7.968*y + t^8.064*y + 2*t^8.28*y + 3*t^8.376*y - t^8.472*y + 2*t^8.688*y + t^8.904*y | t^2.064/g1^12 + t^2.376/g1^8 + g1^18*t^2.904 + t^3. + 2*g1^4*t^3.312 + t^3.72/g1^10 + g1^12*t^3.936 + t^4.032/g1^6 + (2*t^4.128)/g1^24 + g1^16*t^4.248 + t^4.344/g1^2 + t^4.44/g1^20 + g1^20*t^4.56 + t^4.752/g1^16 + g1^6*t^4.968 + t^5.064/g1^12 + g1^10*t^5.28 + (3*t^5.376)/g1^8 + t^5.688/g1^4 + g1^36*t^5.808 - t^6. + t^6.096/g1^18 + (2*t^6.192)/g1^36 + g1^22*t^6.216 + 2*g1^4*t^6.312 + t^6.408/g1^14 + (2*t^6.504)/g1^32 + 4*g1^8*t^6.624 + t^6.72/g1^10 + t^6.816/g1^28 + g1^30*t^6.84 + g1^12*t^6.936 + (2*t^7.032)/g1^6 + (2*t^7.128)/g1^24 + g1^34*t^7.152 + g1^16*t^7.248 + t^7.344/g1^2 + (4*t^7.44)/g1^20 + g1^38*t^7.464 + g1^20*t^7.56 + g1^2*t^7.656 + (2*t^7.752)/g1^16 + t^7.848/g1^34 + 2*g1^24*t^7.872 + t^8.064/g1^12 + t^8.16/g1^30 + g1^28*t^8.184 + (3*t^8.256)/g1^48 + g1^10*t^8.28 + (2*t^8.472)/g1^26 + g1^32*t^8.496 + (2*t^8.568)/g1^44 + (4*t^8.688)/g1^4 + g1^54*t^8.712 + t^8.784/g1^22 + g1^36*t^8.808 + (2*t^8.88)/g1^40 - g1^18*t^8.904 - t^4.344/(g1^2*y) - t^6.408/(g1^14*y) - t^6.72/(g1^10*y) + t^7.032/(g1^6*y) + t^7.44/(g1^20*y) - (g1^2*t^7.656)/y + (2*g1^6*t^7.968)/y + t^8.064/(g1^12*y) + (2*g1^10*t^8.28)/y + (3*t^8.376)/(g1^8*y) - t^8.472/(g1^26*y) + (2*t^8.688)/(g1^4*y) + (g1^18*t^8.904)/y - (t^4.344*y)/g1^2 - (t^6.408*y)/g1^14 - (t^6.72*y)/g1^10 + (t^7.032*y)/g1^6 + (t^7.44*y)/g1^20 - g1^2*t^7.656*y + 2*g1^6*t^7.968*y + (t^8.064*y)/g1^12 + 2*g1^10*t^8.28*y + (3*t^8.376*y)/g1^8 - (t^8.472*y)/g1^26 + (2*t^8.688*y)/g1^4 + g1^18*t^8.904*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46208 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | 0.6616 | 0.8084 | 0.8184 | [M:[1.1009, 0.6974, 1.1009], q:[0.4726, 0.4265], qb:[0.7752, 0.5274], phi:[0.4496]] | t^2.092 + t^2.862 + t^3. + 2*t^3.303 + t^3.605 + t^3.744 + t^3.908 + t^4.046 + 2*t^4.185 + t^4.21 + t^4.349 + t^4.513 + t^4.954 + t^5.092 + 2*t^5.395 + t^5.723 - t^6. - t^4.349/y - t^4.349*y | detail |