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 |
|---|---|---|---|---|---|---|---|---|---|
| 56087 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{7}\phi_{1}q_{1}q_{2}$ | 0.6814 | 0.8689 | 0.7842 | [M:[1.1858, 0.8142, 0.8142, 0.767, 0.767, 0.8378, 0.7906], q:[0.3835, 0.4307], qb:[0.8024, 0.8024], phi:[0.3953]] | [M:[[-6], [6], [6], [-14], [-14], [16], [-4]], q:[[-7], [13]], qb:[[1], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{3}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$ | ${}M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$ | -1 | 2*t^2.301 + 2*t^2.372 + 2*t^2.442 + t^2.513 + t^3.558 + t^3.77 + 3*t^4.602 + 4*t^4.673 + 7*t^4.743 + 7*t^4.814 + 5*t^4.885 + 2*t^4.956 + t^5.027 + t^5.858 - t^6. + t^6.071 + t^6.142 + 2*t^6.212 + t^6.283 + 4*t^6.903 + 6*t^6.973 + 11*t^7.044 + 15*t^7.115 + 14*t^7.186 + 10*t^7.257 + 9*t^7.327 + 4*t^7.398 + 2*t^7.469 + 2*t^7.54 + t^8.159 - 2*t^8.23 - 6*t^8.301 - 6*t^8.372 - 7*t^8.442 - 2*t^8.513 + 3*t^8.584 + 4*t^8.655 + 2*t^8.726 + t^8.797 - t^4.186/y - (2*t^6.487)/y - (2*t^6.558)/y - t^6.628/y - t^6.699/y + t^7.602/y + (5*t^7.673)/y + (6*t^7.743)/y + (8*t^7.814)/y + (5*t^7.885)/y + (2*t^7.956)/y - (3*t^8.788)/y - (2*t^8.858)/y - (3*t^8.929)/y - t^4.186*y - 2*t^6.487*y - 2*t^6.558*y - t^6.628*y - t^6.699*y + t^7.602*y + 5*t^7.673*y + 6*t^7.743*y + 8*t^7.814*y + 5*t^7.885*y + 2*t^7.956*y - 3*t^8.788*y - 2*t^8.858*y - 3*t^8.929*y | (2*t^2.301)/g1^14 + (2*t^2.372)/g1^4 + 2*g1^6*t^2.442 + g1^16*t^2.513 + t^3.558/g1^6 + g1^24*t^3.77 + (3*t^4.602)/g1^28 + (4*t^4.673)/g1^18 + (7*t^4.743)/g1^8 + 7*g1^2*t^4.814 + 5*g1^12*t^4.885 + 2*g1^22*t^4.956 + g1^32*t^5.027 + t^5.858/g1^20 - t^6. + g1^10*t^6.071 + g1^20*t^6.142 + 2*g1^30*t^6.212 + g1^40*t^6.283 + (4*t^6.903)/g1^42 + (6*t^6.973)/g1^32 + (11*t^7.044)/g1^22 + (15*t^7.115)/g1^12 + (14*t^7.186)/g1^2 + 10*g1^8*t^7.257 + 9*g1^18*t^7.327 + 4*g1^28*t^7.398 + 2*g1^38*t^7.469 + 2*g1^48*t^7.54 + t^8.159/g1^34 - (2*t^8.23)/g1^24 - (6*t^8.301)/g1^14 - (6*t^8.372)/g1^4 - 7*g1^6*t^8.442 - 2*g1^16*t^8.513 + 3*g1^26*t^8.584 + 4*g1^36*t^8.655 + 2*g1^46*t^8.726 + g1^56*t^8.797 - t^4.186/(g1^2*y) - (2*t^6.487)/(g1^16*y) - (2*t^6.558)/(g1^6*y) - (g1^4*t^6.628)/y - (g1^14*t^6.699)/y + t^7.602/(g1^28*y) + (5*t^7.673)/(g1^18*y) + (6*t^7.743)/(g1^8*y) + (8*g1^2*t^7.814)/y + (5*g1^12*t^7.885)/y + (2*g1^22*t^7.956)/y - (3*t^8.788)/(g1^30*y) - (2*t^8.858)/(g1^20*y) - (3*t^8.929)/(g1^10*y) - (t^4.186*y)/g1^2 - (2*t^6.487*y)/g1^16 - (2*t^6.558*y)/g1^6 - g1^4*t^6.628*y - g1^14*t^6.699*y + (t^7.602*y)/g1^28 + (5*t^7.673*y)/g1^18 + (6*t^7.743*y)/g1^8 + 8*g1^2*t^7.814*y + 5*g1^12*t^7.885*y + 2*g1^22*t^7.956*y - (3*t^8.788*y)/g1^30 - (2*t^8.858*y)/g1^20 - (3*t^8.929*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50948 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ | 0.6644 | 0.8389 | 0.792 | [M:[1.1879, 0.8121, 0.8121, 0.7717, 0.7717, 0.8324], q:[0.3858, 0.4263], qb:[0.802, 0.802], phi:[0.396]] | 2*t^2.315 + t^2.376 + 2*t^2.436 + t^2.497 + t^3.564 + t^3.624 + t^3.746 + 3*t^4.63 + 2*t^4.691 + 5*t^4.751 + 5*t^4.812 + 4*t^4.873 + 2*t^4.934 + t^4.994 + t^5.879 + t^5.939 - t^4.188/y - t^4.188*y | detail |