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 |
|---|---|---|---|---|---|---|---|---|---|
| 6408 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ + ${ }M_{9}\phi_{1}q_{2}^{2}$ | 0.6901 | 0.8745 | 0.7891 | [M:[1.0269, 0.8206, 1.0269, 0.8206, 1.1794, 0.7175, 0.9731, 1.0762, 0.7175], q:[0.5628, 0.4103], qb:[0.4103, 0.7691], phi:[0.4619]] | [M:[[-22], [-2], [-22], [-2], [2], [8], [22], [12], [8]], q:[[23], [-1]], qb:[[-1], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{9}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{8}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{9}$, ${ }M_{9}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{9}$, ${ }M_{4}M_{9}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}M_{9}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{9}$, ${ }M_{2}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{8}$, ${ }M_{8}M_{9}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{8}$, ${ }M_{4}M_{8}$, ${ }M_{5}M_{9}$, ${ }M_{7}^{2}$ | ${}M_{3}M_{7}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{9}\phi_{1}\tilde{q}_{1}^{2}$ | 0 | 2*t^2.152 + 2*t^2.462 + t^2.919 + t^3.081 + t^3.229 + t^3.538 + t^3.848 + t^3.995 + 5*t^4.305 + 4*t^4.614 + t^4.762 + 3*t^4.924 + 2*t^5.072 + 2*t^5.233 + 4*t^5.381 + 4*t^5.691 + t^5.838 + 3*t^6.148 + t^6.162 + t^6.309 + 9*t^6.457 + 9*t^6.767 + 3*t^6.915 - t^6.928 + 4*t^7.076 + 7*t^7.224 + 4*t^7.386 + 8*t^7.534 + t^7.681 + 8*t^7.843 + 3*t^7.991 - t^8.005 + 8*t^8.3 + 2*t^8.314 - 5*t^8.462 + 15*t^8.61 + t^8.623 + 2*t^8.758 - t^8.771 + 11*t^8.919 - t^4.386/y - (2*t^6.538)/y - t^6.848/y + (2*t^7.305)/y - t^7.466/y + (4*t^7.614)/y + (2*t^7.924)/y + (2*t^8.072)/y + (4*t^8.233)/y + (4*t^8.381)/y + (2*t^8.543)/y + t^8.691/y - t^4.386*y - 2*t^6.538*y - t^6.848*y + 2*t^7.305*y - t^7.466*y + 4*t^7.614*y + 2*t^7.924*y + 2*t^8.072*y + 4*t^8.233*y + 4*t^8.381*y + 2*t^8.543*y + t^8.691*y | 2*g1^8*t^2.152 + (2*t^2.462)/g1^2 + g1^22*t^2.919 + t^3.081/g1^22 + g1^12*t^3.229 + g1^2*t^3.538 + t^3.848/g1^8 + g1^26*t^3.995 + 5*g1^16*t^4.305 + 4*g1^6*t^4.614 + g1^40*t^4.762 + (3*t^4.924)/g1^4 + 2*g1^30*t^5.072 + (2*t^5.233)/g1^14 + 4*g1^20*t^5.381 + 4*g1^10*t^5.691 + g1^44*t^5.838 + 3*g1^34*t^6.148 + t^6.162/g1^44 + t^6.309/g1^10 + 9*g1^24*t^6.457 + 9*g1^14*t^6.767 + 3*g1^48*t^6.915 - t^6.928/g1^30 + 4*g1^4*t^7.076 + 7*g1^38*t^7.224 + (4*t^7.386)/g1^6 + 8*g1^28*t^7.534 + g1^62*t^7.681 + 8*g1^18*t^7.843 + 3*g1^52*t^7.991 - t^8.005/g1^26 + 8*g1^42*t^8.3 + (2*t^8.314)/g1^36 - (5*t^8.462)/g1^2 + 15*g1^32*t^8.61 + t^8.623/g1^46 + 2*g1^66*t^8.758 - t^8.771/g1^12 + 11*g1^22*t^8.919 - t^4.386/(g1^6*y) - (2*g1^2*t^6.538)/y - t^6.848/(g1^8*y) + (2*g1^16*t^7.305)/y - t^7.466/(g1^28*y) + (4*g1^6*t^7.614)/y + (2*t^7.924)/(g1^4*y) + (2*g1^30*t^8.072)/y + (4*t^8.233)/(g1^14*y) + (4*g1^20*t^8.381)/y + (2*t^8.543)/(g1^24*y) + (g1^10*t^8.691)/y - (t^4.386*y)/g1^6 - 2*g1^2*t^6.538*y - (t^6.848*y)/g1^8 + 2*g1^16*t^7.305*y - (t^7.466*y)/g1^28 + 4*g1^6*t^7.614*y + (2*t^7.924*y)/g1^4 + 2*g1^30*t^8.072*y + (4*t^8.233*y)/g1^14 + 4*g1^20*t^8.381*y + (2*t^8.543*y)/g1^24 + g1^10*t^8.691*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4800 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ | 0.67 | 0.8364 | 0.8011 | [M:[1.0216, 0.8201, 1.0216, 0.8201, 1.1799, 0.7194, 0.9784, 1.0791], q:[0.5683, 0.4101], qb:[0.4101, 0.7698], phi:[0.4604]] | t^2.158 + 2*t^2.46 + t^2.935 + t^3.065 + t^3.237 + t^3.54 + 2*t^3.842 + t^4.014 + 3*t^4.316 + 2*t^4.619 + t^4.791 + 3*t^4.921 + t^5.093 + t^5.223 + 3*t^5.396 + 3*t^5.698 + t^5.87 - t^4.381/y - t^4.381*y | detail |