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 |
|---|---|---|---|---|---|---|---|---|---|
| 2840 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ | 0.6544 | 0.8219 | 0.7962 | [M:[0.7069, 0.8399, 0.7069, 0.8399, 1.1601], q:[0.8732, 0.42], qb:[0.42, 0.7401], phi:[0.3867]] | [M:[[14], [-6], [14], [-6], [6]], q:[[-11], [-3]], qb:[[-3], [9]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ | ${}\phi_{1}^{3}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$ | 0 | 2*t^2.121 + t^2.32 + 2*t^2.52 + t^3.48 + 3*t^3.68 + 3*t^4.241 + 2*t^4.441 + 5*t^4.64 + 3*t^4.84 + 3*t^5.039 + 2*t^5.601 + 5*t^5.8 + 4*t^6.2 + 4*t^6.362 + 3*t^6.561 + 8*t^6.761 + 6*t^6.961 + 6*t^7.16 + 4*t^7.36 + 2*t^7.559 + 3*t^7.721 + 7*t^7.921 - t^8.121 + 4*t^8.32 + 5*t^8.482 - 4*t^8.52 + 4*t^8.682 + 3*t^8.719 + 11*t^8.882 - t^4.16/y - (2*t^6.281)/y - t^6.48/y - t^6.68/y + t^7.241/y + (2*t^7.441)/y + (5*t^7.64)/y + (3*t^7.84)/y + (3*t^8.039)/y - (3*t^8.401)/y + (4*t^8.8)/y - t^4.16*y - 2*t^6.281*y - t^6.48*y - t^6.68*y + t^7.241*y + 2*t^7.441*y + 5*t^7.64*y + 3*t^7.84*y + 3*t^8.039*y - 3*t^8.401*y + 4*t^8.8*y | 2*g1^14*t^2.121 + g1^4*t^2.32 + (2*t^2.52)/g1^6 + g1^6*t^3.48 + (3*t^3.68)/g1^4 + 3*g1^28*t^4.241 + 2*g1^18*t^4.441 + 5*g1^8*t^4.64 + (3*t^4.84)/g1^2 + (3*t^5.039)/g1^12 + 2*g1^20*t^5.601 + 5*g1^10*t^5.8 + (4*t^6.2)/g1^10 + 4*g1^42*t^6.362 + 3*g1^32*t^6.561 + 8*g1^22*t^6.761 + 6*g1^12*t^6.961 + 6*g1^2*t^7.16 + (4*t^7.36)/g1^8 + (2*t^7.559)/g1^18 + 3*g1^34*t^7.721 + 7*g1^24*t^7.921 - g1^14*t^8.121 + 4*g1^4*t^8.32 + 5*g1^56*t^8.482 - (4*t^8.52)/g1^6 + 4*g1^46*t^8.682 + (3*t^8.719)/g1^16 + 11*g1^36*t^8.882 - (g1^2*t^4.16)/y - (2*g1^16*t^6.281)/y - (g1^6*t^6.48)/y - t^6.68/(g1^4*y) + (g1^28*t^7.241)/y + (2*g1^18*t^7.441)/y + (5*g1^8*t^7.64)/y + (3*t^7.84)/(g1^2*y) + (3*t^8.039)/(g1^12*y) - (3*g1^30*t^8.401)/y + (4*g1^10*t^8.8)/y - g1^2*t^4.16*y - 2*g1^16*t^6.281*y - g1^6*t^6.48*y - (t^6.68*y)/g1^4 + g1^28*t^7.241*y + 2*g1^18*t^7.441*y + 5*g1^8*t^7.64*y + (3*t^7.84*y)/g1^2 + (3*t^8.039*y)/g1^12 - 3*g1^30*t^8.401*y + 4*g1^10*t^8.8*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 |
|---|---|---|---|---|---|---|---|---|
| 3391 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}M_{6}$ | 0.6685 | 0.8456 | 0.7906 | [M:[0.7228, 0.8331, 0.7228, 0.8331, 1.1669, 0.8331], q:[0.8607, 0.4165], qb:[0.4165, 0.7504], phi:[0.389]] | 2*t^2.168 + t^2.334 + 3*t^2.499 + 3*t^3.666 + 3*t^4.337 + 2*t^4.502 + 7*t^4.668 + 4*t^4.833 + 6*t^4.999 + 4*t^5.835 - 2*t^6. - t^4.167/y - t^4.167*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1824 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | 0.6574 | 0.8268 | 0.7952 | [M:[0.7351, 0.7916, 0.6718, 0.8549, 1.1451], q:[0.8691, 0.3958], qb:[0.4591, 0.7492], phi:[0.3817]] | t^2.015 + t^2.205 + t^2.29 + t^2.375 + t^2.565 + t^3.435 + t^3.52 + t^3.71 + t^3.9 + t^4.031 + t^4.221 + t^4.305 + t^4.39 + t^4.411 + t^4.495 + 3*t^4.58 + t^4.665 + t^4.75 + t^4.77 + 2*t^4.855 + t^4.94 + t^5.13 + t^5.451 + t^5.535 + t^5.64 + 2*t^5.725 + t^5.81 + t^5.895 + t^5.915 - t^6. - t^4.145/y - t^4.145*y | detail |